Upload
others
View
1
Download
0
Embed Size (px)
Citation preview
Diplomarbeit
Titel der Diplomarbeit
On the Counter-Intuitiveness ofQuantum Entanglement
Verfasser
DI(FH) Reinhard Stanzl
angestrebter akademischer Grad
Magister der Philosophie (Mag.phil.)
Wien, im März 2012
Studienkennzahl lt. Studienblatt: A 296Studienrichtung lt. Studienblatt: PhilosophieBetreuer: Univ.-Prof. Dr. Martin Kusch
Contents
1 Introduction 71.1 Setting . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71.2 Goal . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71.3 Method and Structure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
1.3.1 Key Principles . . . . . . . . . . . . . . . . . . . . . . . . . . . . 81.3.2 Experiment . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 91.3.3 Interviews . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 101.3.4 Philosophy . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11
2 Quantum Entanglement 132.1 Einstein, Podolsky and Rosen . . . . . . . . . . . . . . . . . . . . . . . . . 13
2.1.1 Thought Experiment . . . . . . . . . . . . . . . . . . . . . . . . . 132.1.2 Measurement . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 142.1.3 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15
2.2 Schrödinger’s Definition of Entanglement . . . . . . . . . . . . . . . . . . 152.2.1 Definition: Entanglement . . . . . . . . . . . . . . . . . . . . . . . 162.2.2 Epistemological Groundwork . . . . . . . . . . . . . . . . . . . . 162.2.3 Measurement . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 172.2.4 Ψ-function, Catalogue of Expectations . . . . . . . . . . . . . . . 182.2.5 Entanglement by Example . . . . . . . . . . . . . . . . . . . . . . 19
2.3 Interim Conclusion 1 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 202.4 Bell Inequalities and Experiments . . . . . . . . . . . . . . . . . . . . . . 222.5 Interim Conclusion 2 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23
3 Quantum Opto-Mechanics 253.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 253.2 The Experiments . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26
3.2.1 Fabry-Pèrot Cavity . . . . . . . . . . . . . . . . . . . . . . . . . . 273.2.2 Radiation Pressure . . . . . . . . . . . . . . . . . . . . . . . . . . 28
3
Contents
3.2.3 Cantilever . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29
3.2.4 Putting it Together . . . . . . . . . . . . . . . . . . . . . . . . . . 30
3.2.5 Requirements for Success . . . . . . . . . . . . . . . . . . . . . . 31
3.2.6 Paradigmatic Model and Experimental Forks . . . . . . . . . . . . 32
4 The Aspelmeyer Group 354.1 Research Topic and Genesis . . . . . . . . . . . . . . . . . . . . . . . . . 35
4.2 My Relationship to the Group . . . . . . . . . . . . . . . . . . . . . . . . 36
4.3 Facts and Figures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 36
4.4 The Interviewees . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37
4.4.1 Dr. Witlef Wieczorek . . . . . . . . . . . . . . . . . . . . . . . . . 37
4.4.2 Dilek Demir . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
4.4.3 Dr. Nikolai Kiesel . . . . . . . . . . . . . . . . . . . . . . . . . . 38
4.4.4 Mag. Florian Blaser . . . . . . . . . . . . . . . . . . . . . . . . . 39
4.4.5 Dr. Garrett Cole . . . . . . . . . . . . . . . . . . . . . . . . . . . 39
4.4.6 Jonas Hörsch . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40
4.4.7 Prof. Dr. Markus Aspelmeyer . . . . . . . . . . . . . . . . . . . . 41
4.5 Issues Raised by the Interviews . . . . . . . . . . . . . . . . . . . . . . . . 41
5 Counter-Intuitiveness 435.1 General Definition . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
5.2 Specifics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45
5.3 Characteristics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49
5.3.1 By Comparison . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49
5.3.2 Notion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 53
6 Coping 676.1 Aim of Science? Coherent System of Assumptions . . . . . . . . . . . . . 70
6.2 New Generations of Scientists . . . . . . . . . . . . . . . . . . . . . . . . 71
6.3 Bachelard: Reason Instructed by Fabricated Experience . . . . . . . . . . . 73
6.3.1 Pedagogics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 75
6.3.2 Technology . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 77
7 Conclusion 81
Bibliography 87
Appendices 93
4
Contents
A Acknowledgment 95
B Group: Supplementary Notes 97
C Transcription of Interviews 99
D Resume 137
E Abstract 139E.1 Abstract (English) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 139E.2 Abstract (German) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 140
5
1 Introduction
1.1 Setting
Quantum mechanics is claimed to be a very successful theory in physics. However, there is ageneral debate that a deeper understanding of quantum mechanics might still be lacking.1 Ageneral tone of puzzlement, the complications in conveying the theory to the ‘layman’ and asubtle need for repeated re-assurance of the foundations of quantum mechanics in the lightof newly discovered effects can be seen as indicators for such an explanatory deficiencyof the theory. The feature of quantum mechanics which is at the core of this discussionis quantum entanglement. It is appropriate to consider quantum entanglement as the keyeffect of quantum mechanics. On the one hand because it is central to the debate about theuneasiness, or let us say counter-intuitiveness, of quantum mechanics in the past and present.On the other hand because it is the key resource of recent experimental and technologicalendeavors.
To me as a student of philosophy and physics, this is a unique and noteworthy situation intoday’s sciences. It is even more interesting because of the continuing experimental progressof the last few decades. The thought experiments which provoke counter-intuitiveness are,or are on the verge of, being realized by actual experiments. Additionally, this evolutionaryprocess is being propelled by the prospect of yielding new, unprecedented technologies.
1.2 Goal
In order to make this attractive point in time accessible for debate, I will attempt to depicta plausible picture of the situation. Although limited in cogency due to the use of examplesand samples to state the thesis2, I intend to put forward a comprehensive notion of quan-
1 See for instance Bokulich and Jaegger 2010, p.1.2 Especially due to the fact that I have picked one experimental system, interviewed only the people involved,
and I am also being educated at the same Viennese physics institute, it is apt to claim simply local validity.
7
1 Introduction
tum entanglement at the intersection of fundamental counter-intuitiveness and experimentalproduction. Put differently, I will approach the notion of the counter-intuitiveness of en-tanglement by regarding those carrying out the experiments. Doing so will hopefully helpto clarify what is meant by scientists expressing that “quantum mechanics runs counter totheir/our intuition”, to point out which essential intuitions are involved in the actual experi-ments, and what can be revealed about the peculiarities of this counter-intuitiveness.
1.3 Method and Structure
The method, or the general tone in which this thesis is written, is a hybrid one. I intend todepict a stimulating picture of the current situation concerning the counter-intuitiveness ofquantum entanglement by utilizing different types of approaches:
• Introduction of key principles of quantum mechanics using pivotal papers of the earlyyears
• Description of a current experimental system which tackles the counter-intuitive funda-mentals of quantum mechanics
• Exploration of interviews conducted with the people developing and operating this ex-perimental system
• Scrutinizing the statements made in the interviews in the light of key concepts of GastonBachelard’s epistemology
1.3.1 Key Principles
In this introductory section I will put forward the very aspects of quantum entanglement,which challenge the let us say ‘classical’ intuitions. The theoretical grounds on whichcounter-intuitiveness can be pinpointed are depicted by highlighting the major fundamentaldifferences between quantum and classical mechanics. This specifically concerns the dif-ferent understandings of measurement, entanglement, state and property.3 I will refer to theoriginal papers of Albert Einstein et al. (EPR 1935) and Erwin Schrödinger (Schrödinger1935). On the one hand to appreciate the historicity of this topic, and on the other handbecause these initial contributions are very clear-cut and still valid.
A more universal suitability of the thesis is nevertheless not excluded, but might need further support.3 Wave-particle duality will not be invoked due to its rather minor contribution to the understanding of quan-
tum entanglement.
8
1.3 Method and Structure
It is important to record that this thesis follows and rests upon a minimal mainstreamCopenhagen-type interpretation. Other interpretations of quantum mechanics are not re-ally considered here, but will be mentioned selectively. It is my conviction4 that one rea-son why there are a multitude of equivalent interpretations around to date (e.g. variants ofBohm’s mechanics, Many Worlds,...) is that each suffers from distinct points of counter-intuitiveness. These might differ in their specific content, but they are equal in their capacityto violate classical intuition. However, it is sensible to explicate the notion of counter-intuitiveness of quantum entanglement along the lines of the mainstream5 interpretation.It will be the tacit background of this thesis. Distinct tenets which are necessary willbe introduced separately if required for argumentation; for instance Schrödinger’s account(Schrödinger 1935).
1.3.2 Experiment
The entry point of the thesis is a current experiment, or rather an experimental system, whichtries to realize opto-mechanical entanglement. This experimental system is operated by thegroup Quantum Foundations and Quantum Information on the Nano- and Microscale at thefaculty of physics at the University of Vienna, headed by Prof. Dr. Markus Aspelmeyer.6
Their main research objective “[...] is to investigate the quantum effects of nano- and mi-croscale systems and their implications for the foundations and applications of quantumphysics. [Their] goal is to gain access to a completely new parameter regime for experimen-tal physics with respect to both size and complexity.”(Aspelmeyer Group 2011)
This experimental system has been chosen because it incorporates the following features:Firstly, it establishes and studies quantum entanglement, which is the characteristic featureof quantum mechanics, at a size scale close to the ‘classical’ macroscopic world. Henceit questions anew the passage between quantum and classical mechanics.7 Moreover, itsultimate success, i.e. the entanglement of optical and mechanical oscillation, which is closebut has not yet been reached, is a rich soil for anticipating the outcome and contemplating themeaning of the possible results. Secondly, the experimental system poses the fundamentalquestion about the validity limits of quantum mechanics, not explicitly stated by theory and
4 Since I do not have the necessary insights into all interpretations of quantum mechanics, it is more of a pro-found belief. A comparison of the major interpretations with regard to their specific counter-intuitivenesswould be preferable, but is not within the scope of this thesis.
5 At least it is mainstream in the academic education I was schooled in and which I know of from othercolleagues.
6 Henceforth referred to as the ‘group’ or the ‘Aspelmeyer group’.7 For instance, see Schrödinger’s cat (Schrödinger 1935, p.812,vol.48)
9
1 Introduction
hence eminently subject to experimental probing. Thirdly, it nicely illustrates the necessarymastery over technical challenges and limits in order to make the experiments even possible.
For all those general reasons I see this experimental set-up as a typical example for the cur-rent situation in experimental quantum mechanics. Of course, being an example it certainlyhas its particularities. However the idea is to elucidate the questions posed in this thesis bymeans of this example. A vital part of the thesis will thus consist of a non-mathematicalintroduction to this experimental set-up.
1.3.3 Interviews
At the heart of the thesis are the interviews conducted with members of the Aspelmeyergroup. I carried out seven interviews at lengths of about 30 to 45 minutes. The intervieweeswere chosen to be a representative sample of all group members with respect to their aca-demic status and their involvement in the various experiments being currently implementedby the group. I thus interviewed undergraduates, graduates, PhD students, post-doctorateresearch fellows and the group leader. The assortment of the interviews was not carriedout beforehand, but developed during the course of the interviews as it became clear to mewhich people were of interest.
The interviews generally serve two purposes. First they are a viable way of efficiently ap-proaching the group and getting a glimpse of the insights of their structure and their op-erating principles. This will become more apparent in section 4 The Aspelmeyer Group.Secondly, the analysis of the notion of counter-intuitiveness of quantum entanglement willbe backed by reference to the statements of those people who are responsible for the actualexperimental implementation of the nano- and microscale quantum systems.
The interviews were conducted in a very straightforward and frank way, as everybody, in-cluding myself, but excepting the group leader, were novices to interviews. In addition, mylevel of training in quantum physics allowed me to resort to a common ground of knowledgewith the interviewees and hence communicate on a par. There was also no strict adherenceto a questionnaire. Nevertheless, I did prepare a list of questions, but they served rather as acrib sheet and as a crutch so as not to forget to tackle all of the following key issues:
• Age, education and motivation for engaging this area of research
• The hands-on assignment within the group and the actual experiment
• The interviewee’s personal take on the relationship between interpretation, theory andexperiment, especially in this specific case
10
1.3 Method and Structure
• Their personal take on the matter of counter-intuitiveness and how to deal with it
• How does experimenting help in comprehending the subject matter
1.3.4 Philosophy
In order to elaborate the counter-intuitiveness of quantum entanglement in more philosoph-ical detail, I will refer to key concepts devised by Gaston Bachelard. As a French physicist,philosopher and historian of science, active in the first half of the twentieth century, he advo-cated a rationalist constructivist epistemology. Long before Thomas Kuhn’s historicism ofscience and his referral to revolutionary breaks in science, Bachelard became a representa-tive of a French tradition of emphasizing the historical dimensions of science and its ruptures(Nickles 2011). In Le Nouvel Esprit Scientifique (Bachelard 1988), Bachelard argues for thepresence of a shift in the conception of the world in physics, considering the new insightsbrought forth by, for instance, quantum physics. Classical perspectives in physics, as ratio-nal they may have been in their own time, appeared to him to have become an obstacle toprogress in physics. Hence a new spirit of scientific rationale was established in that era.However, Bachelard’s account of discontinuity is not as radical as Kuhn’s. Bachelard speaksof progress and development towards the truth. He strongly stressed the fact that successorparadigms, such as non-Euclidean geometry or quantum physics, conserve their predeces-sors as special cases; particularly in their historical and as a consequence in their pedagogicalcontext. In this regard Bachelard developed an intelligible framework for describing scien-tific thinking and its change at the beginning of the twentieth century. I consider some of hisconcepts to be very fitting for studying the situation of the counter-intuitiveness of quantumentanglement.
First, as a physicist his ideas have a natural proximity to the subject matter. Reading aboutthe pivotal physical examples for a new scientific spirit, such as the rise of quantum physics,conveys the feeling especially with someone literate in physics that he certainly captured therelevant aspects in a comprehensible way. Although Bachelard does not specifically refer toquantum entanglement, his practical ideas of how to make conceptualization intelligible inthis context are very helpful and hence will be deployed in this thesis. In concrete terms,I will make use of Bachelard’s idea of the epistemological profile, and to some extend hisPhilosophy of the No (Bachelard 1980). The former will be applied to quantum entangle-ment in order to show and specify, at the locus of the very notion, the difference between‘normal’ physical terms and quantum entanglement.8 The latter will then be used to further
8 See section 5.3.2 Notion
11
1 Introduction
stress the point by applying the basic idea of Bachelard’s Philosophy of the No to quantumentanglement. In general, the idea is that every comprehension of a (physical) matter is thesum of justified criticism to (i.e. saying no to) a specific, initial and naive picture of under-standing.9 I will show that such an initial, naive picture is far from being intuitive in the caseof quantum entanglement.
The second aspect which makes Bachelard a unique source for the tools used to study thecounter-intuitiveness of quantum entanglement is his type of rationalism. As a consequenceof the analysis of the new scientific mind, Bachelard advocates the idea that it is best de-scribed by a rationalism whose reason is instructed by fabricated experience. I definitelyagree with such an understanding of what happens in physical experimental science eventoday. This becomes apparent when seen in the light of the experiment(s) put forward inthis thesis, especially their dependence on technology and how a phenomenon like quantumentanglement is actually fabricated.10
As a third concept I will also briefly refer to Bachelard’s historicity of science. SpecificallyI will pick up the idea that the historical genesis of the comprehension of a matter is alsoreflected in the pedagogics of the matter. For instance, although Euclidean geometry isonly a special case of non-Euclidean geometry, in teaching we follow the historical order– which is also a philosophical order – from the naive realistic to the growing rationalistunderstanding. Hence for Bachelard, pedagogics connects the historical with the conceptualaspects. This approach will be the background for cues given at the end of the thesis whenasking if and how we should cope with the counter-intuitiveness of quantum entanglement.
Certainly many other philosophers of science have dealt with each of these three aspects aswell; probably in even more detail and depth. The point of restricting this thesis to Bachelardis generally due to the way these philosophical concepts are applied. My intention is not tocompare different philosophical approaches in the light of a case study, namely quantumopto-mechanics. The idea is to utilize a generally fitting and intelligible set of philosophicalconcepts to depict the situation of the counter-intuitiveness of a physical concept, say quan-tum entanglement, represented by the case study. Bachelard’s thoughts make it possible onthe one hand to comprehensibly present the subject matter, but on the other hand also to raisefurther questions pointing beyond this thesis. As an early representative of the philosophyand history of science, Bachelard’s epistemology anticipates many aspects fleshed out by hissuccessors and hence sustains enough topicality to be of relevance for the questions at hand.
9 See section 5.3.2 Philosophy of the No10 See section 6.3 Bachelard: Reason Instructed by Fabricated Experience
12
2 Quantum Entanglement
2.1 Einstein, Podolsky and Rosen
In order to introduce the basis of counter-intuitiveness in quantum mechanics and especiallythat of quantum entanglement, I will roughly retrace the influential key papers of the his-torical developments in this field. The starting point is the paper by Einstein, Podolsky andRosen (EPR) (EPR 1935). By devising a specific thought experiment the authors of theEPR paper intended to show that the quantum mechanical description of physical reality isincomplete. That is to say that not every element of the physical reality has a counterpartin the theory of quantum mechanics. The inability of quantum mechanics to predict themeasurement result of a physical quantity with certainty1 is, according to Einstein et al.,due to the insufficiency of quantum mechanics to consider all relevant variables necessaryto predict a measurement result with certainty. Therefore it is apt to assume a yet unknownhidden variable, which if found and taken into account would yield certain measurementresults instead of the statistical ones put forward by quantum mechanics. Theories followingthis line of thought are called hidden variable theories (HVT).
2.1.1 Thought Experiment
The very core of the EPR paper is a thought experiment which can be paradigmaticallyexplicated as follows:2
For a start we will consider a source which produces two objects, e.g. particles. One is sentto site A, which is commonly called Alice, and the other one to site B, referred to as Bob.Alice and Bob are very far apart; space and time separated. This means that whatever isdone, for instance at Alice, has no immediate influence on what happens at Bob, becausethe fastest possible speed with which an influence could travel from one side to the other is
1 See section 2.2 Schrödinger’s Definition of Entanglement for details.2 For more details see (Mermin 1985)
13
2 Quantum Entanglement
Source
Alice
+
−
+
−
−
+
Bob
−
+
−
+
+
−
1
2
3
4
56
obs:
Figure 2.1: Paradigmatic EPR experiment
the speed of light3. Spacing Alice and Bob so far apart makes it possible to conclude thatmeasurements conducted at Alice can in no way influence the results of measurements atBob, if both measurements are finished in faster succession than light could travel betweenthe two sites. This assumption of the EPR paper is generally called the locality assumption.
The second assumption is about the physical reality of properties. “If without in any waydisturbing a system, we can predict with certainty (i.e. with probability equal to unity) thevalue of a physical quantity, then there exists an element of physical reality corresponding tothis physical quantity.”(EPR 1935, p.777) In other words, if we are able to predict with cer-tainty the result of a non-disturbed measurement, it is fitting to say that the specific measuredquantity existed prior to the measurement.4
2.1.2 Measurement
Our next step is to conduct a series of measurements. Each new run is a sequence of si-multaneously5 measuring the physical quantity of the objects produced at the source andsent to Alice and Bob anew. For reasons of simplification the physical quantity measuredin our example can only result in + or −. At the end we will have obtained two lists, oneof Alice’s measurement results and one of Bob’s; see figure 2.1. Comparing the results ofthe two lists, we apparently recognize that in this example there is a strong anti-correlationbetween the measurement results of Alice and those of Bob. At the first measurement (obs:
3 See Einstein’s Special Relativity Theory (SRT).4 See section 2.2 Schrödinger’s Definition of Entanglement for the differences to quantum mechanics.5 In order to maintain locality.
14
2.2 Schrödinger’s Definition of Entanglement
1) Alice received a + and Bob a −. Analyzing the entire lists, the modest conclusion whichcan be drawn is that whatever we measure at one site, the other site will have the oppositeresult. Due to the assumption of locality, it is impossible that the measurement result knownat one site was somehow sent to the other site and manipulated the measurement there insuch a way as to always show the opposite of the result of the other site. Hence, accord-ing to Einstein et al., the only possibility why we measure such an anti-correlation betweenthe sites, which are so far apart, is that the physical quantity measured was already givenwith certainty at the source of the object prior to the measurement (see reality assumption).Therefore a physical process in the source – which brings about the distinct anti-correlationof the measurement results in each particular case – must be taken for granted.
2.1.3 Conclusion
The core of the matter is that quantum mechanics6, as we will see very soon, describesthe situation and its results, portrayed above, necessarily without the need for a processlocated in the source pre-determining the distinct physical quantities. This circumstanceis primarily owing to its divergent understanding of measurement. From the standpointof Einstein et al., this is exactly why the theory of quantum mechanics is deficient andincomplete. For the sake of having a complete theory, “every element of the physical realitymust have a counterpart in the physical theory.”(EPR 1935, p.777) Quantum mechanics lacksa theoretical representation of the real (i.e. which serves the reality assumption) physicalprocess in the source determining the physical quantities with certainty, which is commonlyparaphrased as the absence of, or the need for, a hidden variable.
How the thought experiment (EPR 1935) is seen from the point of view of quantum me-chanics and its key to a solution, namely entanglement, will be put forward in the light ofSchrödinger’s famous paper (Schrödinger 1935).
2.2 Schrödinger’s Definition of Entanglement
The first person to coin the notion of quantum entanglement was Erwin Schrödinger in his1935 article Die gegenwärtige Situation in der Quantenmechanik in the journal Die Natur-
wissenschaften (Schrödinger 1935). It was a response, or as Schrödinger called it in a foot-note, a confession, to the other famous article of that year (EPR 1935). The approach of un-
6 Be reminded that Schrödinger’s depiction of quantum mechanics is the point of view here.
15
2 Quantum Entanglement
derstanding quantum mechanics, and especially entanglement, put together by Schrödingercan still be considered influential for the current, orthodox7 comprehension of quantum me-chanics. Therefore it is beneficial to provide a compact rundown of Schrödinger’s reasoningin this paper. I will start by picking out the definition of entanglement and then clarify whichpresuppositions are implied.
2.2.1 Definition: Entanglement
“Maximale Kenntnis von einem Gesamtsystem schließt nicht notwendig maximale Kenntnis
aller seiner Teile ein, auch dann nicht, wenn dieselben völlig voneinander abgetrennt sind und
einander zur Zeit gar nicht beeinflussen.”
– Schrödinger 1935, p.826, vol.49
“Maximal knowledge of a total system does not necessarily include total knowledge of all its
parts, not even when these are fully separated from each other and at the moment are not
influencing each other at all.”
– Schrödinger8
2.2.2 Epistemological Groundwork
For Schrödinger, understanding the behavior of a natural object entails experimental dataand some intuitive imagination, say an own image, idea or conception, which can be muchmore detailed than any possible experience. It is comparable to a mathematical structure ora geometric figure. For example, we have a notion of a triangle which can be fully calculatedand determined by only knowing some of the possible determining parts. One side of thetriangle and its two adjoining angles are enough – given the precise concept of a triangle –to determine all the other possible parameters of the triangle, such as the length of the twoother sides, the third angle, the radius of the inscribed circle and so on.
Considering that natural objects are not geometrical figures, it is advisable not to carry thisanalogy too far. That is to say natural objects change with time, so knowing the determin-ing parts and having a proper idea of the object’s behavior in time allows us to calculate
7 Throughout this thesis a minimalist version – meaning in terms of metaphysical statements necessary forreferencing the mathematics with the experimental phenomena – of the Copenhagen interpretation of quan-tum mechanics is considered orthodox or mainstream.
8 Translation by John D. Trimmer, published in Proceedings of the American Philosophical Society, 124,323-38. [And then appeared as Section I.11 of Part I of Quantum Theory and Measurement (J.A. Wheelerand W.H. Zurek, eds., Princeton University Press, New Jersey 1983).]
16
2.2 Schrödinger’s Definition of Entanglement
each future state of the object. In addition, despite having an exact model in the realms ofgeometrical figures, we ought to take notions, ideas or models of the real world more ashypotheses. As in the case of hypotheses, we do not circumvent the arbitrariness inherent inevery notion, but it can be isolated in the presuppositions and from a calculus. The classicalmethod of a precise model aims to improve on isolating the inevitable arbitrariness in itssuppositions by adapting it to the continuing experiences gathered (via experiments).
In summary, for Schrödinger, a model of a natural object is the image or idea and contains,for example, certain laws or relations. Each model has variables, e.g. coordinates, massor speed, which can be observed, or rather measured, and hence are called observables. Astate is the concrete realization, i.e. an instance, of the model with definite values of itsobservables.
2.2.3 Measurement
In a classical, naive realistic view, every observable has a specific value at all times. It mightchange over time, but by looking at it at one moment, i.e. at a certain state, it is fixed.Here the measurement just reads out the value of the examined observable. The inability tomeasure an exact value, or better put, to measure within some margin of error, is due to theimperfection of the measurement process. This naive realistic understanding of measure-ment presupposes the pre-existence of a value of an observable prior to its measurement. Aswe have already seen, this is the understanding Einstein clinged to and hence concluded thatquantum mechanics was not complete in its description of physical reality.9
A totally different notion of measurement is the quantum mechanical one. It does not assumea pre-existing value, but considers that ’only what is measured is real’ and refuses any claimto knowledge prior to the measurement. With this notion of measurement it is possible thatthe observable is not necessarily pre-determined, but has a certain probability of deliveringthis or that value in the cause of a certain measurement. Hence this understanding and therelevant calculus can tell to which degree of prediction accuracy a measurement is feasible.In contrast to the classical view, where imperfections in determining the exact value are dueto the imperfections of the measurement, the fundamental probability of obtaining a certainvalue remains, even given that the measurement is perfect. Schrödinger expresses this differ-ence with an illuminating analogy. “Es ist ein Unterschied zwischen einer verwackelten oderunscharf eingestellten Photographie und einer Aufnahme von Wolken und Nebelschwaden.”(Schrödinger 1935, p.812, vol.48) “There is a difference between a shaky or out-of-focus
9 See section 2.1 Einstein, Podolsky and Rosen.
17
2 Quantum Entanglement
photograph and a snapshot of clouds and fog banks.”
As a consequence of rejecting naive realism, it is correct to presume that an observable ingeneral has no specific value prior to its measurement. Bluntly put, since reality does notdetermine the measurement result, the measurement has to determine reality (Schrödinger1935, p.824, vol.49). This implies that by means of the measurement, the observable be-comes the resulting value. Repeating the measurement will result in the same value; ofcourse within error margins. In a strict sense there is no difference between the naive real-istic and the quantum mechanical view; both fulfill the criteria of returning the same mea-surement result on repetition of the measurement. What type of repetition? So far, repeatingthe measurement is understood as just resetting the measurement device and making a newmeasurement. Sticking to the naive realistic view there is no difference if, in addition toresetting the measurement apparatus, the measured object is also set back to its initial state.Classically, a measurement is not supposed to change a pre-exiting value in the course ofthe measurement (non-interfering measurement) and hence the measured value of the objectis no different whether it is the result of the first measurement or a later one. However, ac-cording to the quantum mechanical view there is a uniqueness to the first measurement ofa system. As the measurement determines the previously unknown, or to be more preciseundetermined, value of the observable, there is no interaction-free measurement and everymeasurement of the same object which follows the first one only replicates the result of thisfirst determining measurement. Consequently, in order to acquire information on how themeasured object and the measurement apparatus interact and which distribution of observ-able values one receives, it is necessary to repeat a series of ‘first’ measurements. This meansthat after each measurement everything (measurement apparatus and measured object) hasto be reset to, or to put it more suitably, re-prepared in its initial state. The result of such asequence of ab ovo measurements is a statistical distribution of the values of the measuredobservable resulting from the interaction between the specific state the measured object is inand the measurement process/apparatus.
2.2.4 Ψ-function, Catalogue of Expectations
The instrument of describing and predicting the probability of these measurement resultsis the Ψ-function. It completely represents the system and can been seen as a catalogueof expectations. From a classical point of view the Ψ-function seems to be incomplete10,because it does not determine which specific value will be the result of the measurement,
10 See section 2.1 Einstein, Podolsky and Rosen
18
2.2 Schrödinger’s Definition of Entanglement
but merely provides the probability of measuring a specific value. However, a specific Ψ-function always has to be considered complete from the perspective of quantum mechanics.This holds true because in quantum mechanics adding a proclaimed unknown observable orhidden variable to the Ψ-function changes it completely. Different Ψ-functions express thatthe system in in different states, while complementary, identical Ψ-functions express thatthe systems are in the same state.
2.2.5 Entanglement by Example
For example, let us assume we have two separated, non-interacting objects, which thus havedifferent Ψ-functions. Now we make them interact and become one system in one state. Inthe classical view we would sum up the properties (specific values of the observables), alterthem by some proper laws of interaction and have a set of properties for the new combinedsystem. Separating the two objects once more would result in two objects with again twoindependent sets of properties. Of course they would not have the same values as before,due to the interaction with each other, but now after the separation they are no longer inter-dependent. This is the understanding of Einstein et al. of the physical process in the sourceof the EPR experiment (see figure 2.1).
From the quantum mechanical point of view, we do not have any pre-measurement values,but probability distributions. Making the two objects interact results in a new Ψ-function forthe total system. As an Ψ-function does not predefine any specific values, there is the possi-bility that due to the interaction of the two objects, the total Ψ-function is comprised of morethan the sum of the two separate ones. To be even more accurate: It is appropriate to saythat if two systems interact with each other, the Ψ-functions do not interact, but they ceaseto exist individually and only one for the total system remains (Schrödinger 1935, p.848,vol.50). This even holds true after the two objects have been separated again. Schrödingerdubbed this phenomenon entanglement.
The following simple example demonstrates this quantum mechanical interrelation betweenthe two systems after interacting (Schrödinger 1935, p.845, vol.50):
q = Q and p = −P (2.1)
This set of equations stands for: If the measurement of the observable q of the first systemreturns a certain value, a measurement of the observable Q of the second system results inthe same value. And the result of a measurement of p in the first system will have the same
19
2 Quantum Entanglement
result as a measurement of P in the second system, but with opposing sign and vice versa.
The measurement of either p or P or q or Q dissolves the entanglement, because as illus-trated above in the section about the quantum mechanical understanding of measurement,measuring determines a specific value and every further measurement yields the same result.Knowing one value renders the entanglement relation useless. If we want to experimentallytest whether this entanglement relation is a good model, we need to make many repetitionsof ab ovo measurements. The results, whatever the actual values are, will show that thereis this kind of entanglement relation (see equations 2.1) between those two systems. Thereliability of this test depends on the amount of repetitions of ab ovo measurements made;the more there are, the more probable is the conclusion of having an entanglement drawnfrom the measurements.
What would be the picture if we remained within the classical naive realistic view? It isalso possible to have a correlation between the two systems after separation as illustratedabove. However, the values exist prior to their measurement. Hence in order to explain thespecific sequence of, in this point of view, certain results of ab ovo measurements, we haveto suppose there is a process controlling this, namely a ‘hidden variable’.
2.3 Interim Conclusion 1
The thought experiment of the Einstein et al. paper (EPR 1935) links the following threefundamental statements about physics in such way that in order to avoid contradiction notall of them can be held to be true. Thus at least one of them must be rendered false.
Completeness: Quantum mechanics is a complete theory. According to the EPR paperthis means in a strict sense that every element of physical reality has its counterpart in thisphysical theory.
Reality: If we can predict with certainty the result of a measurement of a physical quan-tity without disturbing the measured system, then there is an element of physical realitycorresponding to this physical quantity.
Locality: Results of a measurement at one site do not influence the measurement result indistant (space and time separated) sites by any dynamical mechanism faster than the speedof light.
For Einstein et al. the reality and the locality assumption are matters of the very foundationsof physics and are certainly nothing to be abandoned lightly. Therefore they concluded
20
2.3 Interim Conclusion 1
that quantum mechanics does not exhaustively describe physical reality, and opted for theexistence of a hidden variable.
The thought experiment and its showcase of the three contradicting statements is completelydifferently resolved according to Schrödinger’s view of quantum mechanics. As we haveseen, Schrödinger supports a different understanding of measurement and thereby under-mines the classical assumption of reality of the EPR paper. Moreover, and that is the key,by taking the essential principles of quantum mechanics seriously, he ends up with quantum
entanglement. This very notion allows quantum mechanics to give a complete description ofthe physical situation of the EPR thought experiment, but at the cost of subverting the realityassumption and/or the locality assumption. It is not done by blatant opposition, calling thestatements at stake simply false, but by rendering these assumptions irrelevant and pointless.
An important thing to note is that this dismissal of the classical reality and/or the localityassumption was not seen as automatically applying to the entirety of physics. In the earlydays, quantum mechanics was seen as a theory of very small size scales: atoms, particles,and so on. This fact can already be found in the very same paper by Schrödinger. There,besides developing the notion of entanglement, he emphasized the weirdness of applyingthese fundamentals of quantum mechanics to human scale objects by means of his famousSchrödinger’s cat experiment (Schrödinger 1935, p.812, vol.48).
In summary, we have examined two different understandings of how to interpret the EPRthought experiment and what conclusions to draw from it. The Einstein et al. and theSchrödinger perspectives rationally argue in favor of clinging on to fundamental assumptionswhich they want to preserve at the price of having to dismiss others. Both are equal in theirpower to explain the EPR thought experiment. At the time of the emergence of these twoviews there was no instance, preferably experimental evidence, that could decide whichunderstanding was the correct one. Therefore this rather metaphysical question tended to betreated hypothetically and thus did not have the publicity and the verve which we perceive itto have nowadays.11 The actual reason why the EPR thought experiment and the questionsconnected with it gained relevance in the 1970s was the development of a testing scheme(inequality) by John Stewart Bell (Bell 1964). In this way an instance was found that couldexperimentally decide which one of the two perspectives is correct.
11 “[...] (EPR) paper had 36 citations before 1980 and 456 more through June 2003.” (Redner 2005, p.3)
21
2 Quantum Entanglement
2.4 Bell Inequalities and Experiments
The question developed up to now is whether it is possible to understand quantum mechanicsin terms of a hidden variable, thus being a local realistic theory, or not. Despite an early,and to some extent deficient, attempt by von Neumann to prove that it is mathematicallyimpossible to have such a hidden variable in quantum mechanics, it was John Stewart Bellwho devised an inequality to test this question (Bell 1964; Compendium 2009, p.24f). Everylocal realist theory strictly complies with this inequality and quantum mechanics, on thecontrary, violates the inequality. Conducting an experiment which tests the inequality (Bellexperiment) can show that the predictions of quantum mechanics are accurate because theinequality is breached and hence there is experimental affirmation that quantum mechanicscannot be understood in terms of a local realistic theory. In consequence either the localityor the reality assumption, or maybe even both, have to be dismissed or considered pointless.
In 1981 Aspect et al. (Compendium 2009, p.14f) carried out much-noticed experimentsresulting in a violation of the CHSH inequality12 and thereby confirmed that quantum me-chanics is the case. Again, in principle any local realistic theory satisfies the inequality.The experiments show that the inequality is breached. Therefore any local realistic theoryis incapable to account for the experimental results. Whereas quantum mechanics handlesthem very well. Since these first experiments of the CHSH inequality conducted by Aspectet al. in the early eighties, there have been many different types of experiments carried outaffirming the violation of the inequality. (Gröblacher et al. 2007; Rowe et al. 2001; Scheidl2009; Weihs et al. 1998, to name just a few.)
Nonetheless, owing to actual limitations of the experimental capabilities of today, there arestill three types of possibilities to explain the results of these Bell experiments by hold-ing on to local realistic approaches. These categories of loopholes are called Fair Sam-
pling/Efficiency, Freedom of Choice and Locality (Compendium 2009, p.348f). Each ofthese loopholes have been closed individually, and also two of them at once (Quantum 2007;Scheidl 2009). There has been no experimentum crucis excluding all of the loopholes. How-ever, the better and more prudent the experiments are set up, the more complicated and themore devious it becomes to sustain an explanation of these loopholes in terms of a hiddenvariable theory.
12 A derivation of the Bell inequality (Compendium 2009, p.24f)
22
2.5 Interim Conclusion 2
2.5 Interim Conclusion 2
Again, the thought experiment of the EPR paper devises a relation of three fundamentalstatements of physics which renders at least one of them mutually exclusive to the others.Consequently either quantum mechanics is incomplete, measured quantities are not distinctprior to their measurement, or there is something like a superluminal way of interaction.Einstein et al. insisted on the priority of the last two and therefore held quantum mechan-ics to be incomplete. Quantum mechanics, however, here according to the description ofSchrödinger, defines itself very well as complete and consequently rejects the naive under-standing of reality and somehow also locality.
Both points of view refer to the same observable phenomena, i.e. results of the thoughtexperiment. Up until Bell there was no factual experimental criterion to opt for one or theother. He conceived a criterion to distinguish between the predictions of local realistic theo-ries and quantum mechanics (Bell inequality). This made it feasible to conduct experiments,and there have been many of them13 which have certified14 that quantum mechanics is com-plete, as it is able to describe every element of the physical world. The very mechanism,or better say the notion, which derives from the fundamentals of quantum mechanics15 andfully allows us to describe the relevant phenomena, is called quantum entanglement.
13 A very good indicator for the profoundness of the implementation of Bell experiments, at least for me, isthe existence of set-ups for laboratory training of physics students.
14 Of course the loopholes still have to be kept in mind.15 See section 2.2 Schrödinger’s Definition of Entanglement.
23
3 Quantum Opto-Mechanics
3.1 Introduction
A current field of quantum physics which will serve as a showcase and is very illustrative interms of counter-intuitiveness, is quantum opto-mechanics. In order to give a swift insightinto this area, I will start out with a common narrative about the origin or genesis of thisarea of research. It is a short, mostly causal, explanation of why scientists became engagedin this special topic and why “the surf is up”; citing the title of a paper (Aspelmeyer 2010)summarizing the spirit of optimism at a conference in July 2009. Although many papers inthis blossoming field are comprised of similar introductory sections, I will only refer to one(Vitali et al. 2007).
With reference to Schrödinger, the first to coin the term, entanglement is “the characteris-tic trait of quantum mechanics”, and hence the key to the insights of the fundamentals ofquantum physics – indeed of the physical reality – and a resource for the field of quantuminformation processing (e.g. quantum cryptography, teleportation, computing ...). Quantummechanics and consequently entanglement have been situated in the realm of the very small,and extrapolations to the human scale have resulted in odd peculiarities; see Schrödinger’scat (Schrödinger 1935, p.812, vol.48). Up until now experimental expertise and craftsman-ship in quantum physics was limited to the preparation, manipulation and measurement ofphotons, ions, atoms and at best some molecules (Gerlich et al. 2011).
However, in principle quantum mechanics does not pose any limitations to the scale of thesystems to be entangled. Thus, in order to learn more about the fundamentals of quantummechanics – plainly put, the passage between classical physics and quantum physics –, itseems straight-forward to face the challenges of producing entanglement with increasinglylarger macroscopic systems and to test whether one stumbles across any fundamental im-passibility apart from technical ones. Of course there is a large range of systems in physicswhich can be considered macroscopic. Some of them are experimentally workable with cur-rent and near future technologies, including and without further explanation or reference,
25
3 Quantum Opto-Mechanics
single-particle interference of macro-molecules, entanglement between collective spins ofatomic ensembles, or entanglement in Josephson-junction qubits. Nevertheless, the iconicprototype of a ‘classical’ system in physics is the mechanical oscillator, such as a pendulumor a mass on a spring.
Thanks to the huge advancements in microfabrication1 in recent years, it became feasible toproduce micro- and nano-mechanical oscillators with very high precision. How can thesesmall mechanical systems be controlled, i.e. prepared and measured? One obvious approachis to utilize a resource which seems to be well-known2 and well suited for the quantumrealm; photons. Combining these two domains, i.e. setting the mechanical system in motionthrough the radiation pressure of the light and also measuring its movement by light, bringsabout a paradigmatic experiment in the field of opto-mechanics. If it is the goal to attainquantum effects with such a set-up, as is the case here, it is apt to call it quantum opto-mechanics. On a theoretical level, several proposals which were written years before theirtechnical realization was possible describe what has to be done and which parameters haveto be met in order to achieve entanglement for such ‘massive’ systems.
However, a demonstration of quantum effects like entanglement using mechanical oscilla-tors has not been carried out so far. The roadblocks in the way of accomplishing the goalmostly consist of the necessary technology and its stable deployment. Therefore it is fairto say that opto-mechanics is currently in the position of a fast-developing field which is onthe verge of meeting its target. It has rich prospects in terms of applying and furthering theknowledge and skills gathered in its development. Reaching the quantum regime, i.e. see ef-fects specific to quantum mechanics, with macroscopic systems, especially ‘classically’ me-chanical ones, could not only trigger insights into the fundamentals of quantum mechanics,but also improvements and applications in areas like high precision measurement, quantumcomputation and storage, and many more not even conceivable to date.
3.2 The Experiments
The following experimental set-up which is being developed by the Aspelmeyer group con-forms with the very picture of a ‘classical’ mechanical oscillator and nicely fits in with themotives about quantum opto-mechanics presented above. It can be seen as the initial or
1 MEMS or NEMS, as it is often abbreviated, describes electromechanical structures in the scale of micro- ornanometers. The field originated from microelectronics and inherited many of its production toolsets, suchas lithography, etching, doping and so on.
2 The Viennese quantum community has established quite some expertise in setting up experiments whichuse photons as means for showing quantum effects (Quantum 2011b).
26
3.2 The Experiments
paradigmatic experiment. Most of the other experiments currently conducted by the groupare a deduction and advancement thereof.
The general goal of the experiment is to produce quantum entanglement between an opticalsystem, i.e. a stream of photons, and the oscillation of a suspended microscopic mirrorpushed by the radiation pressure of these photons (Vitali et al. 2007).
3.2.1 Fabry-Pèrot Cavity
For a starting point it is beneficial to explain what a Fabry-Pèrot cavity is and does. De-veloped in 1897 it consists of two parallel semitransparent mirrors at a specific distance.Light with a given frequency introduced at one side of the set-up enters the cavity via thefirst mirror, gets partially reflected by the second mirror and thus returns back to the firstmirror, gets partially reflected there, returns again to the second mirror and so forth. Hencemost of the light is reflected back and forth within the cavity. However, the mirrors are onlypartially reflective so some of the light leaves the cavity through the second mirror, i.e. getstransmitted through the cavity. The interesting measurement parameters of this cavity arethe intensity of the transmitted light and the phase shift between the light sent into the cavityand the light leaving the cavity.
Inside the cavity the light waves reflecting back and forth interfere with each other. Depend-ing on the length of the cavity, i.e. the distance between the two mirrors, there is either aconstructive interference and consequently a high intensity of the transmitted light or a de-structive interference which nearly annihilates the transmitted light at the output (see figure3.1).
In other words, the intensity of the transmitted light is very sensitive to the length of thecavity. If the length of the cavity is tuned to constructive interference between the injectedlight and the reflected light, the transmitted light is of high intensity. However, detuning thelength of the cavity by a very small amount destroys the constructive interference rapidly.The tiny shift in the light waves reflecting within the cavity add up to destructive interfer-ences due to the many reflections taking place and each contributing to the growing shiftbetween the injected light and the reflected light in the cavity.
This makes the Fabry-Pèrot cavity a simple, but trusted tool for measuring lengths, refractiveindices of matter, gravity waves3, spectroscopy and so on.
3 E.g. the Laser Interferometer Gravitational-Wave Observatory (LIGO 2011)
27
3 Quantum Opto-Mechanics
Figure 3.1: Interference within the Fabry-Pèrot cavity. Source: SkullsInTheStars 2008
3.2.2 Radiation Pressure
As early as 1871, James Clerk Maxwell theoretically concluded that electromagnetic radia-tion exerts pressure on the exposed surface. This phenomenon was effectively demonstratedby experiments in the early years of the twentieth century (Lebedew 1901; Nichols and Hull1903). However, radiation applies a very weak force on the lighted object, and hence it israther hard to detect. In order to reach the domain in which the radiation pressure is de-tectable, the mass of the lighted object has to be very small and its surface very reflective. Ina simple, classical picture this can be depicted as a stream of photons, meaning light, hittingthe surface like particles with a certain impetus. The impetus of a photon hitting an objectis fully transferred to the object only when the photon is reflected and not absorbed. On alarger scale, the effect of radiation pressure has been shown by the Japanese Aerospace Ex-ploration Agency4. In May 2010 they deployed a spacecraft which as one of its impellentsunfolded a large, thin kite which allowed it to sail with the radiation of the sun (solar wind);similarly to a kite surfer on earth using the wind for propulsion.
4 See (JAXA 2011)
28
3.2 The Experiments
3.2.3 Cantilever
In physics a cantilever is a beam supported only at one end. A simple example for a can-tilever is a diving board. Pushed by a momentary force, it oscillates with its resonant fre-quency. The oscillation diminishes at a certain rate due to external resistances like air drag,but also because of its suspension. A cantilever is a mechanical oscillator, like a pendulumor a spring.
In order to perform experiments which couple quantum optics with macroscopic mechanicaloscillators, it is necessary for the cantilever to meet certain criteria:
• The optical quality of the mirror at the tip of the cantilever has to be very high; i.e. it hasto be very reflective. Over 99.99% of the photons hitting the mirror have to be reflectedand not absorbed. In addition, the light beam hitting the mirror can only be focused toa certain degree, hence the size of the mirror has to be practically somewhat larger thanseveral micrometers (µm) in diameter.
• Each cantilever has a specific oscillation frequency which depends on its size, its form,the material it is made of and its suspension. There are thus many parameters whichhave to be tuned in order to fabricate a cantilever in the desired frequency range. In thisexperimental set-up an oscillation frequency of several megahertz is typical.
• The mass of the cantilever is also essential as it determines the amount of coupling be-tween the light and the cantilever. The smaller the mass of the cantilever, the more theradiation pressure of the light is able to deflect it. Hence small changes in the intensityof the light lead to a strong deflection of the cantilever, and it becomes apt to call themwell coupled. For those reasons it is crucial to minimize the mass of the cantilever, but ofcourse only in respect of the other constraints already mentioned. A typical mass of thecantilevers used is 50 nanograms (ng).
As a consequence of this manifold of essential parameters to be adjusted, it is vital to haveas much control as possible over the process of designing and fabricating the cantilevers.The person who has the skills, expertise and practical know-how to handle this task for thegroup, put also for other groups, is Garrett Cole.5 With a background in material scienceand engineering, unlike the rest of the group, he manages the production of the cantilevers.Another group member who has developed knowledge and skills about the fabrication ofthe cantilevers is Simon Gröblacher. He started to acquire experience in this area during thecourse of his dissertation (Gröblacher 2010), which is about the very experiment presented
5 His interview statements are notable due to his specific assignment, educational background and his uniqueaccess to quantum opto-mechanics.
29
3 Quantum Opto-Mechanics
here. However, because Gröblacher took on a post doctoral position at Cornell Universityand Cole has already been carrying out microfabrication since the turn of the millennium, itis apt to say that Cole is the focal figure concerning the production of the cantilevers for theexperiments.
The actual process of fabrication requires methods well known from computer chip pro-duction and nano technology like lithography, evaporation and etching. Examples of thecantilevers deployed can be found in figure 3.2.
Figure 3.2: a: Scanning electron microscope (SEM) image of a pair of cantilevers(�mirror = 20µm).
b: chip with mechanical resonators of different sizes and shapes. Source:Gröblacher 2010, p.84
3.2.4 Putting it Together
The main idea of this opto-mechanical set-up is to couple the oscillation of the light withinthe Fabry-Pèrot cavity with the mechanical oscillation of a cantilever. In order to accomplishsuch a coupling, we take a Fabry-Pèrot cavity, the length which correlates to the frequencyof the light to have constructive interference. Then we replace the second mirror of theFabry-Pèrot cavity by the small mirror on the tip of a cantilever (see figure 3.3, symbolizedby the mirror with the spring). Henceforth, laser light with a constant frequency enters thecavity through the fixed semitransparent first mirror and reaches the second mirror on thecantilever. The light is reflected from this second mirror and due to the radiation pressure thecantilever is deflected. As a consequence of the deflection of this movable second mirror, thelength of the cavity is detuned. The formerly constructive interference becomes destructiveand the light in the cavity diminishes. In other words, the radiation pressure on the cantilevermirror ceases and the cantilever returns to its initial position. In this way the length of the
30
3.2 The Experiments
cavity returns to the optimum for constructive interference, which is once more the startingpoint for the next iteration of this recurring process.
Figure 3.3: Fabry-Pèrot cavity with movable mirror. Source: Kippenberg and Vahala 2008,p.1172
The outcome of this set-up is the oscillation of the intensity of the light in the cavity, i.e.that there is constructive or destructive interference depending on the deflection of the can-tilever, i.e. the length of the cavity. However, this dependence is not unidirectional, becauseconversely the deflection is reciprocally dependent on the intensity of the light in the cavity.Hence there is an interdependent coupling between the light wave and the deflection of themechanical oscillator.
3.2.5 Requirements for Success
In order to accomplish entanglement it is necessary that the coupling between the opticaland the mechanical regime is larger than the decoherence6 of the two. So the coupling hasto be improved and the decoherence reduced.
The rate of decoherence7 is mainly dependent on temperature. Temperature is motion andas the cantilever is massive it vibrates badly due to its thermal motion. In order to bring thecantilever to its ground state8, it is necessary to cool it close to absolute zero temperature.This is done by placing the cavity including the cantilever in a cryostat9 which cools it to 4K (kelvin). Deeper temperatures such as 20-100 mK (millikelvin) were achieved by using acustom made closed-cycle dilution refrigerator.
The way to increase the coupling between the optical and the mechanical regime is to im-
6 See the concept of decoherence (Bacciagaluppi 2008; Compendium 2009, p.155ff).7 The rate at which the interaction of the system with its environment destroys its quantum state and makes it
classical.8 The system is in its lowest possible energy state.9 A device to maintain cold temperatures. In this case it is a vacuum chamber cooled by liquid helium.
31
3 Quantum Opto-Mechanics
prove the quality of the optical and the mechanical parts. As already mentioned10, the mirroron the cantilever in particular has to have very high reflectivity to utilize almost every photonfor deflecting the cantilever. The mass, shape and suspension of the cantilever (see figure3.2) are also crucial and subject to intensive engineering and development. Moreover, theoptical components like the lasers need proper stabilization, for example by locking theemitted frequencies via feedback. Overall it can be stated that it takes quite an effort to ex-clude environmental influences and to detect quantum entanglement. As pointed out before,entanglement is established in this experimental set-up between the intensity of the light inthe cavity and the deflection of the cantilever. The idea is that if the two observables exhibit acorrelation which cannot be explained classically, entanglement between them has been pro-duced. This means that the two entangled observables can only be described by assumingan indivisible joint state of the intensity of the light and the deflection of the cantilever.
3.2.6 Paradigmatic Model and Experimental Forks
On a fundamental level the opto-mechanical experiments are conducted to show that quan-tum effects can also be found in macroscopic systems. Up to now quantum mechanicaleffects have been demonstrated and utilized in systems of a rather small scale, like masslessphotons, elementary particles, atoms, and up to the size of molecules11. In comparison tothese small entities, a typical cantilever can be seen by the naked eye and consists of in theorder of 1020 atoms12, instead of just a few.
On these grounds it is fair enough to call these opto-mechanical systems macroscopic. Itis a considerable leap forward from the scales with which quantum mechanics has so farbeen tested to be applicable. As already discussed, quantum mechanics does not state anytheoretical limit to its domain of applicability based on size, mass and so on. Of course thereare interactions with the environment which hinder quantum effects13, but circumventingthem experimentally allows us to test the limits of the applicability of quantum mechanics.
However, these main physical principles put forward here do not constitute the full-blownexperimental set-up. They rather have to be understood as something like a general model ormaster form for quantum opto-mechanics. The concrete realizations are a derivation thereof.In the case of the Aspelmeyer group the following set of experiments are conducted to tacklevarying aspects of the topic or to circumvent specific difficulties in the course of implemen-
10 See section 3.2.3 Cantilever11 E.g. fullerene C60 (Quantum 2011c).12 Approximated by assuming that the cantilever consists of 50 nanograms of silicon.13 See concept of decoherence (Bacciagaluppi 2008; Compendium 2009, p.155ff).
32
3.2 The Experiments
tation. This list of experiments worked on by the group members should neither be takenas complete, nor equal in their status, nor in their relevance, nor limited to the group. Theattribution of certain persons to a specific experiment (cited in the brackets) must be takenlightly, as it obscures the presence of mutual assistance and the harnessing of individualskills throughout the group (e.g. see Garrett Cole). Besides all of these shortcomings, it isenough to structure the group.
Master form: This is the implementation of the paradigmatic experiment described above.(Dr. Witlef Wieczorek, Dr. Simon Gröblacher, et al.)
Levitating nano balls: Here the oscillating cantilever is replaced by nano balls held intoposition by the radiation pressure of additional light beams14. (Dr. Nikolai Kiesel, Mag.Florian Blaser, Uros Delic)
Tabletop: A tabletop implementation of the paradigmatic model. The goal is to demon-strate the principles. Reaching the quantum regime, i.e. the occurrence of quantum effects,is not part of this experiment. This project has been developed in the course of a diplomathesis. (Dilek Demir)
Pulsed opto-mechanics: Instead of constantly applying a light beam to the cantilever, it ispulsed. The positive features of this method are the reduced dependency on the tempera-ture of the system and the improved ability to observe space-like separated entanglement15.(Mag. Michael Vanner et al.)16
Coupled cavities: In a collaboration with the Quantum Information Theory Group at theUniversity of Potsdam17 a diploma thesis is under development. The idea is to mechanicallycouple two, and maybe many more, of the cavities described above in order to investigatequantum effects with such more complex systems. It is planned that it will not only compriseof a theoretical examination of the problem, mostly carried out in Potsdam, but also of anexperiment here in Vienna. (Jonas Hörsch, Dr. Garrett Cole)
14 Like a pair of light pincers.15 The cantilever and the pulse of the light are entangled, although they are at different locations.16 This is the only experimental set-up for which I was not able to interview any of the participants. However,
they released a paper on this topic very recently (Vanner et al. 2011).17 Headed by Jens Eisert and Markus Aspelmeyer as one of their visiting professors.
33
4 The Aspelmeyer Group
4.1 Research Topic and Genesis
The key resource of information for this diploma thesis are the people and their currentresearch within the group Quantum Foundations and Quantum Information on the Nano-
and Microscale at the Faculty of Physics at the University of Vienna. Their main researchobjective “[...] is to investigate quantum effects of nano- and microscale systems and theirimplications for the foundations and applications of quantum physics. [Their] goal is to gainaccess to a completely new parameter regime for experimental physics with respect to bothsize and complexity.”(Aspelmeyer Group 2011)
The group originated as a spin-off of the initial research about quantum opto-mechanicsstarted at the Institute for Quantum Optics and Quantum Information (IQOQI 2011). TheIQOQI group around Anton Zeilinger, of which Markus Aspelmeyer was a vital member,innovated and carried out a lot of experiments using photons to demonstrate and utilizequantum effects. Around 2005 the idea came up to also apply this core competence to me-chanical systems. Henceforth Aspelmeyer et al. began their work in the field of quantumopto-mechanics. On the basis of the publication of some initial papers about laser-coolingof micro-mechanical resonators around 2006, it became possible to set out and finance theprojects solely from external funds. In 2009, Aspelmeyer accepted a call for professorship atthe University of Vienna. This resulted in the actual foundation of the group Quantum Foun-
dations and Quantum Information on the Nano- and Microscale at the Faculty of Physicsat the University of Vienna, which Aspelmeyer now heads. Although it was a move fromthe Austrian Academy of Sciences to the University of Vienna it was not a break, but anevolution. It is important to note that there is close collaboration and interrelation among theAustrian quantum research facilities; personnel- and resource-wise. In this case it is nicelyillustrated by the fact that both institutes occupy neighboring buildings connected by a sky-walk. Moreover, a core of the people now leading the experiments within the Aspelmeyergroup started out in the former facility. Despite or even because of that, the actual relocationof the laboratories was only recently completed in April 2011.
35
4 The Aspelmeyer Group
4.2 My Relationship to the Group
I am studying physics and philosophy at the University of Vienna. One of the main reasonsfor me to study physics was the wish to comprehend quantum mechanics and its assertions.Hence I attended various lectures, seminars and talks, some given by Aspelmeyer. In thecourse of developing this diploma thesis it soon became clear to me that I wanted to refer toactual experimental research work. A colleague of Aspelmeyer gave me the tip to ask him,because of his vein for philosophy. I approached Aspelmeyer in December 2010, presentedmy idea and found a sympathetic ear. Early in January 2011 I held a talk to most of the mem-bers of the group, again to present the outline of the diploma thesis and to generally agree oncooperation and on conducting the interviews. I then initially approached Witlef Wieczorekwith a request to introduce me to the experiments and inform me about the relevant literatureneeded to acquire the technical and physical details of the matter.
The contact with the group – all of them are indeed very kind – was kept very modest. Itis important to note that I was never a part of the group and never attended their day-to-daywork. I am an onlooker trying to figure out a comprehension of quantum entanglement on thebasis of their personal statements about the topic. Although this looks like a harsh limitationon the possibilities of gathering information about the group, which is not the primary taskof this thesis anyway, it allowed me to focus on the specific material (the interviews) andthe questions posed. A profound and fair characterization of such a research group wouldindeed demand a greater and longer amount of involvement. On that account the descriptionof the group contains very few observations on my part about the group, and consists almostcompletely of statements by the group members themselves; i.e. the interviews.
4.3 Facts and Figures
In the period the interviews were taken, from May to July 2011, the group consisted of thefollowing 15 people.1
• Prof. Dr. Markus Aspelmeyer (Group Leader) [i]
• Mag. Florian Blaser [i]
• Dr. Garrett Cole [i]
• Uros Delic
1 See Aspelmeyer Group 2011 section ‘People’.
36
4.4 The Interviewees
• Dilek Demir [i]
• Dr. Simon Gröblacher
• Mag. Sebastian Hofer
• Jonas Hörsch [i]
• Dr. Rainer Kaltenbaek
• Dr. Nikolai Kiesel [i]
• Jonas Schmöle, MSc.
• Mag. Alexandra Seiringer (Administration)
• Alexey Trubarov
• Mag. Michael Vanner
• Dr. Witlef Wieczorek [i]
I conducted seven interviews amounting to half of the group, as indicated by [i] in the listabove. In terms of their degrees/qualifications, I tried to pick a representative sample torepresent the under-graduates, graduates, PhD students and post-doctoral research fellowsaccordingly. Another motive for this selection was the assignment of the people to thevarious experiments2.
4.4 The Interviewees
The information presented in this section is a summary of the statements given by the respec-tive interviewees concerning their age, academic career, and assignment within the group.Detailed curricula vitae are available of some of the interviewees on the group’s staff web-site3.
4.4.1 Dr. Witlef Wieczorek
Wieczorek is a thirty-two year old post-doctoral research fellow, who studied physics at theTechnical University of Berlin (TU Berlin) and graduated with a diploma thesis on quantumdots. He worked for four years as a post-graduate on multi-photon entanglement at the
2 See section 3.2.6 Paradigmatic Model and Experimental Forks.3 See Aspelmeyer Group 2011 section ’People’.
37
4 The Aspelmeyer Group
Ludwig Maximilian University in Munich (LMU Munich) (Interviews 2011d, §4).
In his regular curriculum he did not encounter the issues of different interpretations in quan-tum mechanics. However, at a summer school held by Reinhard Werner and Jens Eisert atthe TU Berlin he was introduced to the EPR problem and the Bell experiments (Interviews2011d, §10-13).
In the Aspelmeyer group, Wieczorek is responsible for the realization of the paradigmaticexperiment using cavities with mirrors on cantilevers. Until of late he worked together withSimon Gröblacher, who wrote his dissertation on this experiment and is now Post-Doc at theCalifornia Institute of Technology. Currently Wieczorek is teamed up with Jonas Schmöleet al. on this experiment (Interviews 2011d, §31-32).
4.4.2 Dilek Demir
Demir is twenty-two years old and an undergraduate. After studying physics at the Univer-sity of Vienna, she was, at the time the interview was held, finishing her diploma thesis onradiation pressure effects on macroscopic systems (Interviews 2011a, §5,9,11).
Although she had never heard of quantum physics before studying physics, she quicklybecame attracted by quantum mechanics. Instead of attending some boring lectures, shestarted reading papers and books about the topic; such as the EPR thought experiment.Beyond that, Demir also attended together with some of those who are now her colleagues,the extra-curricular Monday lectures on quantum physics which back then were organizedby Aspelmeyer (Interviews 2011a, §23).
Her assignment, and also the topic of her diploma thesis, is the development, i.e. design,build-up and measurement, of a kind of table-top implementation of the paradigmatic exper-iment, in order to nicely demonstrate radiation pressure. It is not set up to show any quantumeffects, but aims at simplicity and yet precision (Interviews 2011a, §11-15).
4.4.3 Dr. Nikolai Kiesel
Kiesel is a thirty-four year old post-doctoral research fellow who studied physics at theLudwig Maximilian University in Munich (LMU). He joined the Zeilinger group in Viennafor his diploma thesis on three-photon entanglement4 and his dissertation on four-photon
4 On the W state, because the GHZ state (Greenberger, Horne, Zeilinger) has already been implemented inVienna.
38
4.4 The Interviewees
entanglement. In 2008 he moved to the Aspelmeyer group (Interviews 2011c, §16).
He did not become drawn into this area of physics until almost at the end of his studies. Aseminar held by Harald Weinfurter, who at that time worked with the Zeilinger group, gothim interested in the experimental field of quantum mechanics (Interviews 2011c, §4, 13).
Kiesel started up and is currently heading the experiment on utilizing levitating nano ballsinstead of mirrors on cantilevers. His collaborators are Florian Blaser and Uros Delic. Ad-ditionally Kiesel participates in managing and representing the group (Interviews 2011c,§19,23,30).
4.4.4 Mag. Florian Blaser
Blaser is a post-graduate and thirty years old. He started studying physics at the University ofNeuchâtel (Schwitzerland) and came to the University of Vienna in 2005 to write his diplomathesis on the simulation of mechanical systems. Except for some time after graduationworking in the software industry, he has been part of the opto-mechanical experiments sincethe very beginning with Zeilinger’s group. Now he is doing his PhD with the Aspelmeyergroup (Interviews 2011f, §6-12).
Blaser became interested in quantum entanglement and read some books about quantuminformation, which was not well covered in his small home university. While reading therelevant papers he discovered that the group at the University of Vienna was very active andsuccessful in this field of research. Hence he applied successfully to write his diploma thesiswith the Zeilinger group (Interviews 2011f, §16).
Blaser works together with Nikolas Kiesel and Uros Delic on the experiment using levitatingnano balls. At the time of the interview he was programming LabView5 to automate andimprove the measurement process. Anyhow, he like almost all other experimenters is alsooccupied with setting up and aligning the optics, the electronics, and so on (Interviews 2011f,§31,38-39,43).
4.4.5 Dr. Garrett Cole
Cole is a thirty-two year old research fellow who is a sort of a lateral entrant to the group. Hehas a bachelor’s degree in materials engineering from California Polytechnic State Univer-sity. In addition he went to the University of California, Santa Barbara to study electronics
5 Graphical programming environment to develop measurement, test and control applications.
39
4 The Aspelmeyer Group
and photonic materials. Cole completed his PhD in 2005 on MEMS-Tunable Vertical-CavitySemiconductor Optical Amplifiers. After graduation, he was employed for a year in the in-dustry and for two years at the Lawrence Livermore National Laboratory (LLNL Centerfor Micro- and Nanotechnology). Since October 2008 he has been working at the AustrianAcademy of Sciences and the University of Vienna (Interviews 2011b, §5-7).
Cole is well-qualified and experienced in the area of nano- and micro-fabrication, includ-ing design and implementation. His dissertation was on mechanically tunable diode lasers,which are in some ways similar6 to the paradigmatic set-up in quantum opto-mechanics.In the course of his employment at the LLNL Center for Micro- and Nanotechnology, hebecame more and more interested in the physical fundamentals of his work. After readinginto the topic, he came across the work of Aspelmeyer and contacted him. As a result, acollaboration was initiated which had Cole, while still working at the LLNL, fabricate var-ious samples of nano-mechanical devices for testing in Vienna. In 2008, due to a lack ofperspectives at the LLNL, he seized the opportunity to finally join the Viennese quantumcommunity (Interviews 2011b, §7-11).
Although Cole is mainly located within the Aspelmeyer group, his skills and expertise inmicro-fabrication are also made use of by other groups and collaborations. At the time theinterview was held he was engaged in building a test bench to characterize, quantify andoptimize the mechanical response of the fabricated cantilevers, prior to deploying them inthe more time-consuming experiments (Interviews 2011b, §27-31).
4.4.6 Jonas Hörsch
Hörsch is a twenty-five year old undergraduate studying physics at the University of Potsdamas a member of the Quantum Information Theory Group around Jens Eisert. He recentlystarted work on his diploma thesis, which is about mechanically coupled micro-cavities. Itis a cooperation between the Eisert and the Aspelmeyer groups, as there are also plans to testthe theoretical findings on these coupled systems experimentally7 (Interviews 2011e, §3-9,15).
At this early stage in his diploma thesis, Hörsch is still mainly acquiring insights into thedesign and simulation of the mechanical components and the experimental environmenthere in Vienna. However, as a first step he and Cole have already designed some initial
6 They also consist of a cavity, but which is tuned by moving the small mirrors to change the cavity length.The deflection of the mirrors due to radiation pressure, as exploited in quantum opto-mechanics, has beenan unwanted side effect in the context of these lasers.
7 I.e. micro-fabrication by Cole
40
4.5 Issues Raised by the Interviews
prototypes, whose production is to be launched soon (Interviews 2011e, §21-31).
Hörsch was introduced to and became interested in quantum information theory via the lec-tures of Jens Eisert. The University in Potsdam mainly concentrates on the theoretical elabo-ration of quantum information theory and hence lacks the scope of its application. Thereforehe joined the field of quantum opto-mechanics and collaborates with the Aspelmeyer group(Interviews 2011e, §37).
4.4.7 Prof. Dr. Markus Aspelmeyer
He is thirty-seven years old and a professor at the University of Vienna. Aspelmeyer studiedat the Ludwig Maximilian University in Munich (LMU) and later on also studied philosophyat the Munich School of Philosophy8. He took a bachelor’s degree in philosophy and wrotehis diploma thesis and dissertation in physics about the investigation of structural phasetransitions of crystals (solid-state physics). Always up for a challenge, he switched his areaof research after graduation and became Post-Doc with the Zeilinger group in Vienna. Since2009 Aspelmeyer has been Professor of Physics at the University of Vienna and head ofthe Quantum Foundations and Quantum Information on the Nano- and Microscale group(Interviews 2011g, §8-11).
His self-proclaimed main task is to interact and communicate with his group as much aspossible. For that reason he tries to be in the laboratories and lend a helping hand wheneverpossible. In this way Aspelmeyer tries to provide new impulses to the group and set thecourse of the research. Another main part of his work is of course to keep the funding forall the experiments pouring in (Interviews 2011g, §21-25).
4.5 Issues Raised by the Interviews
After having introduced the interviewees with regard to their academic vita and assignmentin the group, it is time to illustrate the key topics which emerged in the course of the inter-views. The central issue is certainly the counter-intuitiveness of quantum entanglement, butthe emphasis of its analysis is strongly oriented towards the answers given by the intervie-wees. The two key topics which I discerned from the entirety of the interviews and whichwill serve as my work order for the rest of the thesis are the following:
Counter-intuitiveness: With certain nuances, the interviewees had difficulties in putting8 Hochschule für Philosophie München
41
4 The Aspelmeyer Group
their tentativeness about the matter into words. Certainly the more educated, involved andinterested in these fundamental questions about the comprehension of quantum mechanicsa scientist is, the more she is able to express and discuss the topic at hand with precision.In short, the group leader is of course more articulate with regard to the subject than anundergraduate. On these grounds it seems appropriate to develop a fitting account of thecounter-intuitiveness of quantum entanglement. Firstly by introducing a very general def-inition of counter-intuitiveness.9 Secondly by carving out the specifics regarding quantumentanglement as introduced at the beginning of the thesis10, and thirdly by characterizing thespecific counter-intuitiveness by employing key epistemological thoughts from Bachelard.11
Coping: A key issue for the interviews was the question of whether experimenting helps inovercoming the difficulties of comprehension. The short and superficial answer is probablyno. However, this certainly demands a more detailed examination. Abstracted to a morecomprehensive level, the issue raised is how to generally cope with the counter-intuitivenessof quantum entanglement. Does science and do scientists need to cope with it? 12 What basicconsiderations can be spelled out concerning the possibility of experiments being of assis-tance in evolving our reasoning in order to accommodate the difficulties of comprehendingthe matter? 13
Again, this extraction of the central issues tackled within the interviews not only summarizesthe main content of the interviews, but can also be regarded as a motive for the elaborationswhich follow. Moreover, relevant quotes from the interviews will be deployed as evidencefor supporting particular arguments. Hence the further study of a definition of counter-intuitiveness and the handling of the counter-intuitiveness will rest on three pillars: Theactual context of quantum opto-mechanics and the respective experiment previously intro-duced, the perspectives expressed in the interviews, and the set of tools consisting of keyconcepts of Bachelard’s epistemology.
9 See section 5.1 General Definition.10 See section 5.2 Specifics.11 See section 5.3 Characteristics.12 See section 6.1 Aim of Science? Coherent System of Assumptions.13 See section 6.2 New Generations of Scientists and 6.3 Bachelard: Reason Instructed by Fabricated Experi-
ence.
42
5 Counter-Intuitiveness
5.1 General Definition
In principle there is nothing exceptional about the term “counterintuitive”. Every sensiblelanguage user knows the meaning of this adjective and makes more or less frequent use ofit in the proper context. Nonetheless I will first spell out a definition and then continue fromthere. According to the Merriam-Webster dictionary, counterintuitive means that somethingis “different from what you would expect”. In the same dictionary, the term is described assomething “not agreeing with what seems right or natural” (Merriam-Webster 2011a).
Hence the adjective counterintuitive labels facts and circumstances as not corresponding towhat one has assumed. If, as the second definition implies, the expected appears to be rightor natural, it is a slippery slope which I am not inclined to travel. In the case of quantumentanglement, but also very generally in science, claims of justification based on what seemsright or what seems natural are very problematic. Thus it is sufficient to initially concentrateon the function of the adjective counterintuitive to indicate a difference between an issueand what we have expected about the issue.
How central this idea of countering is will become clearer by studying the difference be-tween it and something which can be called non-intuitive. At first glance the latter is used tomanifest the case of not having any intuition, and hence any expectation, at all with regardto the subject matter. For instance, it seems close to impossible to actually form an intu-ition about higher dimensional (higher than three dimensions) or warped (curved) spaces.1
However, on second thoughts calling something non-intuitive in normal parlance has a verysimilar usage pattern as counterintuitive. If a subject matter is not intuitive, it is also notaccording to our expectations. Therefore the difference between non- and counter-intuitive
appears to be a matter of gradation. Calling something non-intuitive is a weak indicationof its non-conformance with intuition. By contrast, labeling something counterintuitive is a
1 Some mathematicians might claim to have developed an intuition about those constructs. This is definitelysomething worth taking a closer look at, but certainly not in this thesis.
43
5 Counter-Intuitiveness
much stronger claim that our intuitions are contradicted by the subject matter. We use it tostate that a matter of fact is in conflict with, or resists, our intuitions. Basically it is a term toemphasize the problematic nature of a contradiction between intuition and a matter of fact.
Another approach to a general understanding of counterintuitive springs from a definitionof intuition. In general, again according to the Merriam-Webster dictionary, intuition is“a natural ability or power that makes it possible to know something without any proof orevidence” (Merriam-Webster 2011b). Taking a look at entries on intuition in other booksof reference (Encyclopaedia Britannica 2011; EnzyklPhilWiss 2010; Rorty 1967), allows usto, probably more universally, define intuition as an immediate apprehension.
The key to this definition of intuition is to consider immediate in two ways here. At firstwe can of course think of it in a more chronological manner, i.e. something is assumed orknown from intuition due to the unavailability of distinct proof or evidence. That is, we drawon intuitions about a subject matter owing to a lack of knowledge about it. However, as soonas there is sufficient proof or evidence, i.e. some process of gaining additional knowledgeand inference is involved, the intuition either dissipates, becomes irrelevant or is definitelyvalidated as justified, unjustified, right or wrong. In this way the intuition is marginalized orsuperseded as soon as there is relevant proof or evidence. Hence no matter if the intuitionand the subject matter do coincide or not, we might not care anyway, as proof or evidenceis valued much higher in this case. Supposing that intuitions are not in accordance with thefacts of the matter, we might be inclined to use the weaker label non-intuitive here.
The second way of considering the immediacy in the definition of intuition is in a, let ussay, logical manner. In contrast to adopting intuitions as a placeholder which are supersededby more knowledge about the matter, intuitions in this sense function as more immediateaccess to the matter in parallel with proof or evidence. Hence it is not a question of whenthe intuition has been formed or whether the knowledge about the subject matter is alreadyin place, but rather the idea that the immediacy of the apprehension in the course of havingintuitions is relevant. If, as in our instance, intuitions do not coincide with our availableknowledge of the matter, we can make the strong case for labeling them counterintuitive.This means that we allow the immediacy of our intuitions to be considered enough to maybeeven challenge or cast doubt on the available proof or evidence.2
In sum, the point I wish to make here is that counterintuitive not only qualifies a subject mat-ter as being not in accordance with our immediate apprehension (= intuition) of the matter,but especially emphasizes its problematic contrariness. How this understanding specifically
2 Certainly this is only the case if the speech act is not considered an empty phrase. For instance, expertsbragging about the unintelligibility of the matter in order to intimidate or impress non-experts.
44
5.2 Specifics
applies to the counter-intuitiveness of quantum entanglement will be studied in the followingsection.
5.2 Specifics
A way to provide a generally conclusive definition of counter-intuitiveness in the realm ofquantum entanglement which is suite to the subject is unfortunately not that straightforward.One of the major difficulties is that a definite contradiction between a concrete intuition anda specific datum of quantum mechanics strongly depends on the respective interpretation ofquantum mechanics and its corresponding assumptions. This means that a specific elabo-ration of the counter-intuitiveness of quantum entanglement is bound to and only valid inthe light of the interpretation chosen. For instance, the notion of quantum entanglementonly makes sense in a couple of interpretations of quantum mechanics. Thus, the notionof counter-intuitiveness in the realm of quantum mechanics first of all indicates that there issome sort of conflict between intuitions and scientific facts and that is the only commonplacewhich can be generally stated. Again, how this contradiction manifests itself in detail hingesvery much on the specific understanding or interpretation of quantum entanglement actuallyput forward.
In this thesis, as already mentioned, the presentation of the counter-intuitiveness of quan-tum entanglement will be carried out against the background of a somewhat mainstreamCopenhagen-type interpretation. In order to be even more precise, I consider the descriptionof quantum mechanics by Schrödinger (Schrödinger 1935) sufficient for the task. Other in-terpretations of quantum mechanics are not considered in this thesis, because I am convincedthat each (e.g. variants of Bohmian mechanics, many worlds ...) individually contains a cer-tain sore point of counter-intuitiveness. This means that although their content is different,they all share the peculiarity of challenging fundamental intuitions which are classicallyheld about the world. An interpretation not burdened with counter-intuitiveness would bethe most probable candidate for quickly becoming the general doctrine in this field. Asthis is not the case, it is sensible to take the notion of the counter-intuitiveness of quantumentanglement for its function of generally marking a contradiction between a theoreticalor experimental phenomenon in quantum physics and common intuitions about the world.However, in order to analyze the notion it has to be studied in a specific context, say adoptingthe perspective of a certain interpretation; as the following will show.
We will briefly recall the core issue introduced in the preceding part of this thesis to begin
45
5 Counter-Intuitiveness
with. The central EPR thought experiment is basically comprised of three statements whichcannot be simultaneously true. Hence at least one of them is mutually exclusive to the oth-ers, or meaningless in a way. First, the completeness assumption: A theory is complete inthe strict sense that every element of physical reality has to have an appropriate counterpart,i.e. must be represented in the theory. Second, the reality3 assumption: If we are able topredict with certainty the result of a measurement of a physical quantity without disturb-ing the measured system, then there is an element of physical reality which corresponds tothis physical quantity. Third, the locality assumption: Measurement results at one site donot influence the measurement results in far apart (space and time separated) sites by anydynamical mechanism faster than the speed of light. Einstein et al. relied on their knowl-edge and their intuitions about the classical physical world and insisted on the validity ofthe two assumptions about the reality and the locality of physical phenomena. Therefore,due to the cogency of the thought experiment they concluded that quantum mechanics – indescribing the EPR thought experiment – cannot be complete. Again, assuming two of thethree statements to be true excludes the other. As the theory of quantum mechanics cannotbe considered complete in the eyes of Einstein et al., they proposed fixing it by generallyextending the theory by a hidden, not necessarily known, variable.
In contrast, quantum mechanics, here according to the description of Schrödinger, is per-fectly complete as a theory and there is no need for – or even more strongly, it strictlyforbids – the assumption of hidden variables being a part of it. All physical phenomenaare properly describable by quantum mechanics, although new concepts like quantum en-tanglement are the consequence. Now that the completeness of quantum mechanics is thepivotal requirement, one or both of the other assumptions (reality, locality) of the thoughtexperiment have to be circumvented, invalidated or rendered meaningless.
Both points of view refer to and explain the same observable phenomena, i.e. results of thethought experiment, but differ with regard to their counter-intuitiveness. As can easily beseen, the position of Einstein et al. is perfectly consistent with the common, classical intu-itions about the physical world; namely the reality of physical quantities independent of theirmeasurement and the impossibility of instantaneous4 impacts of simultaneous measurementsconducted far apart. Quantum mechanics does, however, contradict or render meaninglessthese common classical intuitions and hence can be regarded as counterintuitive.
3 The notion of reality certainly has huge implications in the philosophy of science. It is definitely not myintention to touch upon any of the vast discussion about reality and its various understandings. Here realis used in a very naive physical sense. In this context it rather means that the value of a physical quantity isdetermined at any given time independently of its measurement. This applies throughout the thesis.
4 With respect to Einstein’s special relativity theory, superluminal.
46
5.2 Specifics
Besides the difference in such soft criteria like compatibility with common intuitions, therewas no factual reason to pick one over the other. It was John Stewart Bell who conceiveda criterion (Bell inequality) to test differing predictions of classical hidden variable theoriesand the theory of quantum mechanics. A great number of experiments (Bell experiments),conducted during the last four decades affirmed5 that statements made on the basis of thetheory of quantum mechanics are the case. Any hidden variable theory is inherently unableto accommodate for the experimental data produced. Consequentially, hidden variable the-ories, although tending to be rather immediately intelligible and intuitive, are ruled out dueto experimental evidence. In reverse the theory of quantum mechanics is experimentallyunderpinned, but does not coincide with common intuitions about the world.
Hitherto this does not sound like a very unusual situation for modern day science. Manyscientific theories are not compatible with the respective common intuitions held about theworld. In addition, despite the fact that the compatibility of a theory with everyday intuitionscan be a criterion for the actual theory choice, much like simplicity or beauty, fortifiedevidence arguably has more weight in this respect. However, the counter-intuitiveness ofquantum entanglement may not be different to other counterintuitive theories in principle,but it certainly is in gradation. The specific trait of the situation of quantum entanglement isthat the intuitions contradicted by evidence are the most fundamental ones. They are sucha fundamental part of our comprehension (perception) of the world that doubting them isindeed imaginable, but nevertheless close to impossible to conceive. This is not only thecase for the layman, but also for the people involved with (experimental) research. Forexample, statements like the following are not in a minority among those interviewed forthis thesis.
“I reckon one will never understand entanglement.” 6
– Witlef Wieczorek, (Interviews 2011d, §83)
Even in a more detailed account we can easily see a fundamental difficulty in expressing theissue. Moreover, it becomes apparent that it is not a settled matter, but demands constantrethinking. Which is a nice indicator that something is not as expected; and thus correspondswith the previously introduced definition of being counterintuitive.
“There are a lot of question marks in quantum mechanics. And theoretically it is interest-
ing, because matters normally evident do become not so evident any more. So in the EPR
experiment for example, you have to read the paper twenty thousand times and you still won’t
understand it. Because there is always something in there you didn’t see before. And it is
rather interesting to me that you can always find something you have to understand anew. It is
5 The loopholes have to be kept in mind of course. (Compendium 2009, p.348f)6 Translated by the author.
47
5 Counter-Intuitiveness
somehow this contradiction: It should be like this, but quantum mechanics says it is different.
But why? And then you can start pondering about it. I find that pretty cool.” 7
– Dilek Demir, (Interviews 2011a, §45)
The relationship between puzzlement and our intuitions, as well as the perception of quan-tum entanglement as being counterintuitive, is even more directly expressed by this quote:
“We are simply used to the fact, out of intuition, that if a body has some property, this property
is actually there. Or that it is somehow indeed realized. This has to be totally dismissed with
quantum mechanics. Rather, many properties are not determined before a measurement was
made. [...] Hence the phenomena are counterintuitive. Well, you can somehow imagine them,
but? The maximum one can do is to get used to it.” 8
– Jonas Hörsch, (Interviews 2011e, §61)
These quotes just hint at the intricate understanding and the limited means to accuratelyarticulate one’s personal puzzlement. On a more general level, the substance of the counter-intuitiveness of quantum entanglement comes to light when we take a look at the core ideaof quantum opto-mechanics9 which the experiments of the interviewee are based on.
The exciting momentum of quantum opto-mechanics is its implementation at size scaleswhich are close to the human everyday world. This is basically due to two reasons: First,it underlines the theoretical independence of quantum effects with respect to the size of thesystem it is realized with. Secondly, it also reveals the question of where to draw the linebetween the classical realm and the quantum realm; if there is one.
In detail, as already shown in the very implementation of quantum opto-mechanics in theparadigmatic experiment introduced in this thesis10, the starting point is a mechanical oscil-lator. In our case it is a cantilever of nano scale which is easily comprehensible in classicalmechanical terms. First, it is fitted with a little mirror on its tip and mounted as one partof a cavity (two opposing mirrors). Next, laser light is introduced into the cavity, whichtravels back and forth between the two mirrors. The light in the cavity interferes with itsown reflections. Depending on the length of the cavity, the light oscillating interferes eitherconstructively or destructively, and accordingly the intensity of the light is higher or lower.However, as one mirror of the cavity is the cantilever, it becomes deflected by the radiationpressure of the light. The higher the intensity of the light, the higher the deflection of thecantilever. As the cantilever is deflected, the length of the cavity changes, and consequently
7 Translated by the author.8 Translated by the author.9 See section 3.1 Introduction.
10 See section 3.2 The Experiments.
48
5.3 Characteristics
the interference changes, thereby changing the intensity of the light in the cavity. This againleads to a modification of the deflection and hence the modification of the cavity length.Thus the circle is complete. In sum the experiment realizes a correlation between the inten-sity of the laser light and the displacement of the cantilever. Up to now this is very easilyintelligible solely by the use of classical terms. However, after excluding all of the interfer-ing disturbances (e.g. by extensive cooling and suspension) the correlation between thosetwo observables, the intensity of the light and the deflection of the cantilever, will cease tobe classically explainable. The coupling produced between the optical and the mechanicalregime emerges entangled. That means that the very same conclusion which Schrödingergenerally reached when devising quantum entanglement can be realized here11 with a sys-tem normally conceived as classical. The cantilever, an emblem of classical mechanics, hasbecome a matter of quantum effects at size scales visible to the naked eye.
This specific experimental set-up, besides other things, comprises the counter-intuitivenessof quantum entanglement. Its intention is to realize quantum effects with commonly acces-sible concepts (cantilever, cavity, radiation pressure, ...), and accordingly runs into resultsnot expected in the common classical comprehension of the physical world. Certainly ac-cording to the approach of quantum mechanics, the results of the experiments are altogetherexpected. However, the crux of the matter is that the classical way we commonly apprehendour world leads us to label the results of the experiments counterintuitive. This conceptof counter-intuitiveness is, of course, not restricted to the specific implementation of experi-ments yielding quantum effects, but can also be characterized on a more general level; whichwill follow next.
5.3 Characteristics
5.3.1 By Comparison
When studying intuitions more closely, it often turns out that they are mostly not referredto in a positive way. Either they are commonly mentioned as a last resort for minimaljustification in the absence of any evidence or proof of a matter. Or they are deployed todismiss something as specifically implausible and irrelevant. For instance, using the non-compliance of a subject matter with our intuitions as a knockout argument in debate. In otherwords, intuitions are mostly silently at work in our perception and judgement of the world.They surface most obviously when they conflict with contradicting beliefs or empirical data.11 It is safe to be modest as the actual realization has not been accomplished yet.
49
5 Counter-Intuitiveness
Hence the most apparent form of intuitions is when something is counterintuitive. This iswhere one usually becomes aware of intuitions.
I would like to put forward the following two familiar examples to illustrate the situation.The first one concerns the Müller-Lyer illusion; probably the most famous geometrical-visual trick (see figure 5.1).
Figure 5.1: Müller-Lyer Illusion. Source: Illusionism.org 2008
We came to realize, e.g. through measurement or by believing the testimony of others pre-senting us with the illusion, that the lengths of both lines (without the arrows) are equal.However, we visually perceive the upper line to be shorter than the lower one. Thus it is in-tuitively backed to claim that the lengths of the lines are different. Although we have perfectknowledge about the illusion, i.e. that it is a visual trick and what the correct comprehensionof it ought to be, it is not possible to overcome our intuition about it. It is very important tonote that intuition in this case is equated with the conditions of the human sense of vision,including physical and psychological characteristics. This may not be permissible, or is atleast up for debate. Nevertheless, the point to be made with this example is not where theintuition comes from, but thta it is an intuition denoting the situation of something seeming
to be the case to a person. George Bealer stresses the seeming as the important differencebetween an intuition and a belief (DePaul and Ramsey 1998, p.208). In the Müller-Lyerillusion it still seems to the viewer that one of the lines is longer than the other, althoughshe neither infers nor believes in the difference in length. Bealer points out that the seemingpersists in spite of the countervailing belief.
The second example will not only bolster, but also broaden the understanding of traits ofintuition. In nearly every physics class this experiment is conducted to demonstrate the lawsof free falling objects. Of course there is a whole lot to know and say about the laws offree fall in terms of physics and the history of science. What we will specifically look at isthe following tricky question: If you drop a feather and a steel ball from the same height,
which one will hit the ground first? The common intuition in this case can be describedas follows: It seems to the person asked that the steel ball is heavier than the feather; ittherefore falls faster and hence hits the ground first. This is exactly the doctrine of Aristotle
50
5.3 Characteristics
and scholasticism, criticized for instance by Giovanni Battista Benedetti12 and refuted byGalileo Galilei’s work.
The physically correct answer demands a counter question to clarify the environment ofthe set-up; and that makes the initial question so tricky. Is the fall set up in a force freeenvironment, except for gravity, or not? For example, the case of dropping a feather and asteel ball in a vacuum13 results in both hitting the ground simultaneously. Conducting thesame experiment in a medium like air would result in the steel ball hitting the ground earlier,because the feather suffers more air drag due to its shape. A law-like statement would soundlike this: Without any forces14 in place, except gravity, all bodies, independent of mass,shape and material, fall with the same rate of acceleration and hence hit the ground at thesame moment if dropped from the same height.
This is presumably the most well-established and millionfold experimentally demonstratedfact in physics. Every person who has ever had physics classes in her life is expected tohold this belief, or science education would have failed its assignment big-time. However,it can be denied that the intuition about heavy objects falling faster is eradicated by thisbelief. When asked unexpectedly, let us say brutally woken from well-deserved sleep at 3o’clock in the morning, many people, even the well educated, are not immune from givingthe intuitive answer. This does not indicate that we gave the intuitive answer just becausethe correct belief slipped our mind. The situation is rather that intuition is more immediateand belief is always in need of some contemplation. Immersion in environments wherethe correct conception of the case is very visible, or familiarization (for example throughrepetitive reflection of the case) might reduce the need for contemplation. We will return tothis matter in due course (see section 6 Coping).
The reason why I referred to the free fall example is because many more people are ableto personally relate to the intuitiveness of it than to the perspective of quantum mechanics.Thus it is a beneficial undertaking to highlight the parallels of these two cases.
The starting point is the phenomenon of the different velocities of falling objects in air. Theanalogon in the case of quantum entanglement would be the EPR thought experiment. Ineach case there are basically two hypotheses explaining the phenomenon. In the free fallexample, the Aristotelian and the Galilean. On the quantum entanglement side there is the
12 He devised a simple thought experiment to disprove the scholastics: Connecting two falling balls witha (mass-less) rod does not change the velocity of fall, although the overall mass of the body increases(O’Connor and Robertson 2009).
13 A gravitational field is implicitly assumed, as without it there would be no fall at all.14 Like resistances (e.g. air drag) or magnetism.
51
5 Counter-Intuitiveness
Free fall Quantum entanglementPhenomenon Objects falling with different
speeds (in air)EPR thought experiment
Hypotheses Aristotle vs. Galileo Einstein vs. SchrödingerExperiment Galileo, school experiments Bell experimentsInvalidated Aristotle Einstein
(all local realistic theories)Intuitive Aristotle Einstein
(all local realistic theories)Counter-intuitive
Galileo Schrödinger
Table 5.1: Structural comparison of the free fall example with the quantum entanglementcase.
Einstein picture and the Schrödinger picture. In addition there are experiments by Galileoand Bell which in each case flatly invalidate one of the hypotheses, namely the Aristotelianand the Einsteinian picture. However, both experimentally excluded hypotheses are thosethat are closely related to prevailing intuitions. Hence both cases, i.e. the free fall exampleand quantum entanglement, are a matter of counter-intuitiveness.
Unfortunately, like all good analogies this one also has to come to an end. Although the freefall example shares its form of counter-intuitiveness with the quantum entanglement case, itis very well appeased by another intuition. Here it is air drag, which is not much less intuitiveand commonly accessible. The physically correct description of free fall in air does indeedconflict with the direct intuition of heavier objects falling faster, but is perfectly intelligibleusing the other everyday life concept of air drag. This means that gaining a very simple pieceof additional knowledge, like the existence and resistance of air drag, marginalizes the wrongintuition about objects which fall faster.15 The distinction to the quantum entanglement caseare the intuitions violated; e.g. the reality and locality assumption have no proper intuitive
alternative. Thus far these fundamental intuitions have only been rationally negated andhence this situation is far from being reconciled with a common perception of the world.There is nothing similar in the quantum entanglement case to what the intuition of air dragdoes in the free fall case.
The ongoing search for a more fitting interpretation of quantum mechanics is a good indi-cator. For instance, assuming physical objects without properties prior to their observationor “spooky action at a distance” (EPR 1935) are hard to comprehend without a plausible
15 This classical example is very well comprehensible in terms of the definition of intuition as the absence ofproof and evidence. See section 5.1 General Definition.
52
5.3 Characteristics
story that relates it to the commonly perceived world. This intricacy of the situation not onlymanifests itself at the level of countering intuitions, but can also be shown in the very notionof quantum entanglement.
5.3.2 Notion
After carving out some of the characteristics representative for the counter-intuitiveness ofquantum entanglement, we will now take a closer look at the notion itself. Up to now weestablished counter-intuitiveness along the lines of a phenomenon which contradicts ourclassical expectations instructed by the world we live in (e.g. see reality and locality as-sumption). However, as the notion of quantum entanglement arose from this situation, it isvery suggestive to wonder whether counter-intuitiveness finds its expression in the compre-hension of the notion alone. The tool box I am going to use in order study this matter isequipped with, to my mind, suitable conceptions of Gaston Bachelard’s epistemology.
Introduction to Bachelard’s Epistemology16
Bachelard generally assumes science to be an alternation between empiricism and rational-ism. Instead of both extremes being in diametric opposition, he perceives it as a dialecticrelation. Bachelard argues that an empiricism is always in need of clear, deductive lawsin order to be conceivable and teachable. In addition, a rationalism is not very convincingwithout credible evidence and applications in reality. Hence in order to prove the value of anempirical law, it has to become a basis for logical considerations. Vice-versa, a logical con-sideration becomes admissible when it can become the basis for an experiment. ThereforeBachelard does not advocate a dualism, but a dialectic relation where one is complementedby the other. For him, scientific thinking is to enter the epistemological area between theoryand practice, mathematics and experience. In order to comprehend a law of nature scientif-ically, it is necessary to understand it as both, a phenomenon and a noumenon17 (Bachelard1980, p.20f).
Although this relation between empiricism and rationalism is balanced per se, Bachelarddetects a privilege in contemporary physics in direction of rationalism proceeding to expe-rience. His cue is the rise and the weight of mathematical considerations in current physics.This analysis can also be deemed valid for today’s physics. Mainly because much of today’s
16 This introduction is a rendition of the prologue (Bachelard 1980, p.17-30).17 Caution: not Kant’s noumena (Ding an sich), but rather the general idea about something that can only be
recognized by the mind
53
5 Counter-Intuitiveness
physics relies conceptually on ideas which arose in the period Bachelard is referring to; thefirst half of the twentieth century. Moreover, the very subject of this thesis is a prime ex-emplar for what he calls applied or prospective rationalism18. At the very beginning thereis a rational consideration, say the EPR thought experiment or quantum entanglement, im-posed by other tenets founded in known facts, e.g. blackbody radiation (Compendium 2009,p.39f). Then this rational consideration becomes the subject of a program of experimentalrealization. On the surface, a thought experiment is mostly intended to explicate a theory(or make another theory look preposterous); as in the EPR case.19. Hence there is no needfor realisation in the first place, except in the mind. That is probably one reason, besidesthe technical hurdles, why it took quite some time until an experimental realization was fi-nally devised in the case of quantum entanglement; see the Bell experiments. Furthermore,it is not the blunt implementation of the physical setting of the EPR thought experiment thatmatters, but the realization of the rational idea behind it. Namely to scrutinize whether quan-tum entanglement is the consequence of specific non-classical assumptions (see Schrödinger1935) or proof for the deficiency of quantum mechanics within the framework of classicalassumptions (see EPR 1935). The Bell experiments clearly20 realize quantum entanglementas a phenomenon and the consequence of non-classical assumptions.
According to Bachelard, not only the phenomenon is necessary for scientific comprehension,but also the noumenon. What is the noumenon of quantum entanglement? Is it a clear-cut ra-tional term knowable by its physical definition alone? Where does the counter-intuitivenessof quantum entanglement come into play? Is it inherent to the very notion? The instrumentof choice for answering these questions is the concept of the epistemological profile devisedby Bachelard.
Epistemological Profile
In the book Philosophy of the No, Bachelard explains the idea of the epistemological profile(Bachelard 1980, p.55ff). Hiss starting point is to call into question the generality of therealism held by scientists. Is a scientist a realist in all her thoughts and conjectures? Doesone and the same mind deal with differing gradations of realism in its thinking? Besides,do these gradations depend on the notions concerned, the progression of the beliefs andthe theoretical concepts of the prevailing era? According to Bachelard, a specific notion
18 Rationalisme prospecteur (Bachelard 1980, p.21)19 The scientific tool of the thought experiment is certainly more complex than put forward here (Brown and
Fehige 2011)20 Again, the loopholes concerning Bell experiments have to be kept in mind. (Compendium 2009, p.348f)
54
5.3 Characteristics
is always characterized by a pluralism of philosophical cultures or aspects with divergingweights. The epistemological profile is an instrument to illustrate the psychological effectswhich different philosophical positions have on understanding a notion. An explanation canbe offered based on Bachelard’s own example, the notion of mass:
Bachelard distinguishes five basic philosophical approaches which condition the differentaspects of our personal application of the notion of mass. Naive realism, positivist empiri-cism, Newtonian or Kantian rationalism (classical), complete rationalism (relativistic) andhis dialectic rationalism. At first glance this really looks like a fatal contraction of the vastand diverse field of philosophy into five branches. Nevertheless, if we pay attention to theanalogy Bachelard had in mind, then his approach becomes more reasonable. Think of thevisible spectrum of light from violet to red; it is a continuous spectrum. Each color mergesinto the neighboring one and provides all different kinds of shades of color. The sameapplies to all the possible shades of philosophies. However, within the spectrum of light,pure spectral colors21 are identifiable. In an analogous way, Bachelard designates five basicphilosophies which allow us to categorize the vast spectrum of philosophies. It is implicitwith his approach that the categories devised are not very clear-cut and in turn also consistof a spectrum of different shades. Just as yellow implies all different kinds of yellow.
Again, the visual depiction of the epistemological profile is intended to illustrate the relativerelation of the five philosophies to each other on the x-axis, like a spectrum. The differentvalues on the y-axis of the graph account for the different frequencies of usage, which canalso be interpreted as a relative measure for the relevance of our beliefs regarding this notion.Exact values are of no matter here because, according to Bachelard, such an epistemologicalprofile always refers to a specific notion held by a specific personal mind in time and space.Only a complete collection of the epistemological profiles of all fundamental terms couldbecome the object of what he calls philosophical spectral analysis, which for Bachelardwould be the basis for a comprehensive psychology of the scientific mind. Admittedly wewill not get that far here, but will use the epistemological profile as an instrument to reflect onthe comprehension of counter-intuitive notions; specifically that of quantum entanglement.
To begin with, we promptly introduce Bachelard’s very accessible example of the notionof mass. In principle, almost every person should be capable of sketching her own epis-temological profile of her personal scientific understanding of the notion of mass throughintrospection. Just like Bachelard, we will take the profile given in figure 5.2 as a commonone for our time and culture. Such an assumption is appropriate because in this regard not
21 Colors that are caused by a relatively narrow frequency band of light in the visible spectrum. Violet, blue,green, yellow, orange and red.
55
5 Counter-Intuitiveness
(1)
naive realism
(2)
positivistempiricism
(3)
Newtonianor Kantianrationalism
(4)
completerationalism(relativistic)
(5)
dialecticrationalism
Figure 5.2: Epistemological profile. Source: Bachelard 1980, p.57
much has changed, although more than seven decades have already passed since his writ-ing. In addition, the most frequent usage of the notion of mass will nowadays resort to aNewtonian or Kantian rationalistic understanding (3). This is what is mainly taught in ourgeneral education system, namely classical mathematics and elementary physics (classicalmechanics).22 Nevertheless, it must be granted that growing importance has been laid onthe relativistic understanding of mass by the likes of Einstein.23 Anyway, it is still not thataccessible, as the classical rationalism described before is very pervasive24. Hence a com-pletely rationalistic (relativistic) understanding of mass accounts for a smaller share (4). Thepositive empirical comprehension of mass is of course strongly represented (2). Weighing isan activity which is not only important to science, but also widespread in our daily lives. Itrelates a distinct number to a distinct mass.25 The scrutinizing glance at the bathroom scale,a frequent routine for many, is a telling form of behaviour in this regard. Besides, from timeto time we do think of mass in a naive realistic way (1). Namely in metaphors where werelate mass to nothing concrete but an undefined amount of some quantity. For instance amass of apples, without weighing them or putting them in any rationalist scientific context.This involves a naive realistic understanding of mass; like just stating that there ‘a lot ofapples’. The smallest share in this spectrum is held by dialectic rationalism (5). This isprobably the hardest one to circumscribe, because it is precisely the openness and dialecticbetween phenomenon and noumenon which Bachelard tries to advocate. The details of this
22 Inertial mass is a quantitative measure of an object’s resistance to the change of its speed. Gravitationalmass is a measure of magnitude of the gravitational force. Classically, the equivalence of both types ofmass is noted but not explicated.
23 See special and general theory of relativity.24 As indicated by its height in the y-axis.25 The physical concept of weight refers to a property of matter related but not equal to mass. Weight is
the gravitational force acting on an object. Its mass is an intrinsic property of this object independent ofgravity.
56
5.3 Characteristics
will become clearer by the end of this chapter. For now a possible example, which was notwithin the scope of Bachelard’s considerations because of its newness, is the role and thesearch for Higgs boson as a hypothetical massive elementary particle predicted by the Stan-dard Model. The so-called Higgs mechanism describes how elementary particles obtain theirmass. We could think of it as a good example of how to envision the relationship betweenrationalization and realization in the sense of Bachelard. For the simple reason that it is aprofoundly rational consideration within the Standard Model which, of course among othermotives, triggered the building of the largest machine to this day in order find the origin ofmass.26
Epistemological Profile of Quantum Entanglement
Bachelard’s example of the epistemological profile of the notion of mass seems to be quiteemblematic for many of our foundational terms. What would an epistemological profileof quantum entanglement look like? Bachelard does not consider it directly, but in a shortpassage (Bachelard 1980, p.121) he indicates which unusual characteristics a epistemologi-cal profile of the Heisenberg uncertainty principle would have. As the uncertainty principleis fundamental for quantum mechanics, we will see that it is apt to take up these specificsmentioned by Bachelard and transfer them into the epistemological profile of quantum en-tanglement: Namely Bachelard denies that the Heisenberg uncertainty principle has anyrealistic relevance in everyday life. The same can be said about quantum entanglement, buteven more so.
Two other sources are available for constructing the epistemological profile: my personalcomprehension of the notion of quantum entanglement and the statements of the intervie-wees regarding this topic. It is important to recall that Bachelard’s epistemological profileis a spectrum of the personal psychological effects of the different (philosophical) schemesoperating in conceptualization. Although it is a matter of the individual mind, it is alsolocalized in an intellectual culture of the respective period and community. Hence the epis-temological profile of the notion of quantum entanglement which will be devised here isadmittedly deduced from my personal understanding. Nevertheless, as a student of physics Iam trained in quantum entanglement to a degree that is standard for the people scientificallyinvolved with this topic. Thus I find myself as part of the community at issue in this regard,especially when drawing on the people I interviewed in the course of this thesis. They arethe ones conducting opto-mechanical experiments and hence are engaged with the notion of
26 see Cern 2011.
57
5 Counter-Intuitiveness
quantum entanglement not only theoretically, but also empirically.
Of course the questions and the answers in the interviews concerning this topic do not havethe analytic precision implicated by the instrument of the epistemological profile. They aremore about the general nature of quantum mechanics and the difficulties in understandingit properly. However, they strongly hint at what the epistemological profile of quantumentanglement should eventually reproduce. One very representative quote is the following:
“I already dealt with the Bell inequality, and so on, in my diploma thesis. That is the ‘classical’
example within the quantum mechanical context. And yet, to this day, I have to reconsider it
from a changing perspective again and again. Yet, you have to understand what is happening
there once again. I think that is the fascinating part. Because you can’t lay your finger on what
quantum physics really is. And how to speak about it properly. Therefore you have to develop
so many different models in your mind.” 27
– Nikolai Kiesel, (Interviews 2011c, §32)
An understanding of this kind and the difficulties in conceptually grasping quantum entan-glement are characteristic and can be adequately expressed by the peculiar epistemologicalprofile to follow (see figure 5.3). Not because I am able to assign the exact true weights tothe different columns of the spectrum, but because I reconstruct the structure in a reasonableway, i.e. the relation of negative and positive values, of the profile. This is thus where Iwould locate counter-intuitiveness in this matter; namely in the context of the single notion.
(1)
naive realism
(2)
positivistempiricism
(3)
Newtonianor Kantianrationalism
(4)
completerationalism(relativistic)
(5)
dialecticrationalism
Figure 5.3: Epistemological profile of quantum entanglement.
Like Bachelard with the Heisenberg uncertainty principle, I will draw the naive realistic (1)aspects of the profile with a negative value. There is nothing in everyday life that wouldbring about an intuitive comprehension of quantum entanglement. Moreover, there is no
27 Translated by the author.
58
5.3 Characteristics
meaningful usage of the term in everyday life as there is with the notion of mass. At firstglance it can be argued that the value should be zero. This would signal that the naiverealistic perspective would not matter at all. However it does, because the experience andthe thinking common to our daily life also preforms our scientific mind. This is also inline with Bachelard, because for him each ‘column’ in the spectrum can be regarded asan epistemological obstacle to the others. We have to take this seriously in the case ofquantum entanglement. It is not just that there is no everyday life experience of quantumentanglement, but common knowledge about daily life contradicts the findings of the theoryand the experiments concerning quantum entanglement. In order to take this into account, anegative value is assigned to naive realism.
The same considerations also apply to Newtonian or Kantian rationalism (3) because, as hasbeen shown throughout this thesis, there is a fundamental contradiction between the classicalassumption about realism and/or locality and the fundamentals of quantum mechanics. Ow-ing to the Bell experiments there is also evidence that theories assuming a hidden variableto accommodate for the more intuitive assumptions of reality and locality do not hold true.However, it (psychologically) remains a vital part of the notion of quantum entanglement,but in a negative sense. Again, as with naive realism, Newtonian or Kantian rationalism asthe philosophy of classical physics is incompatible with quantum entanglement, and is thusa resistive element in the spectrum, and a negative value is assigned to it.
The positive empirical comprehension (2) concerns the experiments conducted with quan-tum entanglement, or rather their measurement results. It ranges from the Bell experimentsto the more complex set-ups of late, such as in the field of quantum opto-mechanics. A goodindication of why this perhaps deserves a rather high value is that quantum entanglement isnot only a primary fundamental phenomenon which is being investigated, but also a meansexploited in various applications. Examples of this are quantum teleportation, quantum en-cryption and quantum computing. The experiments realize quantum effects with commonlyaccessible concepts28. It is the results, or let us say the results in the light of the theory,which are non-classical and hence counterintuitive. In general, for quantum entanglement itis a correlation of two observables.29 In the case of the paradigmatic experiment of quantumopto-mechanics featured here, it concerns the entanglement, i.e. non-classical correlation,of the intensity of the light in the cavity and the deflection of the cantilever.30 More generallyin the words of two of the interviewees:
28 For example see cantilever, cavity, radiation pressure, and so forth in the paradigmatic experiment of thisthesis.
29 See the definition of quantum entanglement in section 2.2 Schrödinger’s Definition of Entanglement30 See section 3.2 The Experiments
59
5 Counter-Intuitiveness
“In the moment when you stand in front of the experiment you are indeed always dealing with
classical apparatuses.” 31
– Nikolai Kiesel, (Interviews 2011c, §39)
“So I’m doing classical physics [sarcasm]. The hope behind the experiment is to really go into
the quantum regime.”
– Florian Blaser, (Interviews 2011f, §53)
From this it appears that we have to consider the status of the positivist empirical perspectivetwofold. On the one hand, most of the experimental apparatuses involved and the readingsof the instruments are classically intelligible. They are not in conflict with naive realism (1)or Newtonian or Kantian rationalism (3). Hence on this level there is no contradictory rela-tionship between those three philosophies [(1), (2) and (3)], and the epistemological profileshould tend to look like that of mass (see figure 5.2). That means all three perspectives,naive realism (1), positive empiricism (2) and Newtonian or Kantian rationalism (3), arenon-contradictory and hence all positive. However, on the other hand the final outcome ofthe experiments (i.e. the conclusion of the measurement readings as quantum entanglement,as already shown), contradict the account of naive realism (1) and of Newtonian or Kantianrationalism (3).
In order to somehow incorporate this twofold situation with regard to experiments dealingwith quantum effects, the relationship between the three philosophies [(1), (2) and (3)] isdevised as shown in figure 5.3. The perspective of positive empiricism (2) is drawn witha high positive value in order to appreciate the positivist concentration on the empiricalreadings of classical instruments, as is also the case with quantum experiments. However,the contradiction of the experimental outcome to a naive realistic (1) and a Newtonian orKantian rationalist (3) point of view is expressed by the relation of the positive (2) to thenegative (1) and (3). Of course this adds to the previous arguments which already made usassume the naive realistic (1) and the Newtonian or Kantian rationalist (3) perspective to benegative on their own account.
The completely rationalist or relativist perspective (4) is to my mind difficult to properly takeinto account. On a theoretical level, quantum mechanics has not yet been adequately recon-ciled with Einstein’s general theory of relativity. Apart from that, the Copenhagen interpre-tation of quantum mechanics has a tendency to introduce relativity at the point of measure-ment. As the determination of the property value of a particle is a matter of measurement, itcan be comprehended as being relative to the measurement itself and the measurement con-
31 Translated by the author.
60
5.3 Characteristics
text.32 In sum, this aspect of the epistemological profile of quantum entanglement appears tobe neither very tangible nor very conclusive to me. Due to these shortcomings and its ratherminor importance for the overall argument, I cautiously assess it to be of low relevance.33
On the contrary, dialectic rationalism (5) is considered to be of high value. We do not haveto fully comply with Bachelard’s understanding of this aspect in the epistemological profile.For a start, we can conceive of it more modestly as the very comprehension which scientistsengaged in this field have about quantum entanglement; aside from all the other momentain the spectrum of the epistemological profile. In concrete terms, this contains for instancethe underlying assumption of quantum entanglement that particles do not possess definiteproperty values prior to their measurement. And that the correlation established by quantumentanglement is independent of the distance between the objects involved. Schrödinger’sdefinition of quantum entanglement principally also falls into this category. For now, thisis only a quantitative enumeration of statements about what scientists consider quantumentanglement to mean, besides the difficulties involved with the classical understanding.
In order to study some of the qualitative aspects of this dialectic rationalism, it eventuallybecomes necessary to take a closer look at Bachelard’s Philosophy of the No. This will alsoallow us to once again stress the difference between the counter-intuitiveness of quantumentanglement and that of other scientific notions.
Philosophy of the No
Bachelard wrote a short and accessible introduction to his Philosophy of the No (Bachelard1980, p.155ff). Generally speaking, it is not an appeal for plain negation as an end in itself. Itis a reasonable criticism, i.e. expressing a substantiated no against a given understanding of amatter, which is neither an arbitrary negation, nor a negation without evidence, nor rushinga negation out of principle. What it rather implies is a strong synthetic and constructiveimpetus.
Examples for Bachelard are the panning out of Newtonian mechanics as a special case ofnon-Newtonian mechanics (i.e. the theory of relativity), the Euclidean within non-Euclideangeometry, and so on. In these cases, the negation of key assumptions of the initial theorydid not make them incorrect, but allowed them to be synthetically superposed in a morecomplete understanding. As Bachelard puts it, there is no automatism which would allow
32 This is generally referred to as the so-called measurement problem in quantum mechanics.33 Nonetheless, this aspect is very underexposed here and would deserve more attention beyond the scope of
this thesis.
61
5 Counter-Intuitiveness
us to logically reduce the new tenets to the old ones (Bachelard 1988, p.13f). For himthey are true irreversible extensions not only to the matter, but also to the scientific mindcomprehending it.
Therefore, as a means of generalization and conceptualization, the philosophy of the no re-tains what it negates. The example Bachelard refers to is the notion of the atom (Bachelard1980, p.159f). Nowadays the most common intuitive image of the atom, mentally and pic-torially, is a simplified version of Bohr’s model. It basically resorts to an analogy with themodel of the planetary system. The naive realistic picture is that the electrons circle aroundthe nucleus on defined paths due to electrostatic forces, just as the planets orbit the sun dueto gravitational forces. This is a nice and intuitively accessible picture, but one we are notentitled to take too literally from a scientific perspective. For instance, according to Heisen-berg’s uncertainty principle the electrons are not explicitly locatable on their way aroundthe nucleus. This is just one of the many more adaptations to the model needed in order tosatisfy other physically relevant tenets. Concerning the notion of the atom, Bohr’s model istherefore merely the starting point for an application of critical scientific thinking that dis-misses, i.e. says no to, an ever growing number of details implicated by the original material.Increasing scientific knowledge about the atom therefore increases the divergence betweenthe initial intuitive image and the current scientific comprehension of the notion of the atom.
The essential insight of Bachelard is that the actual notion of the atom always retains a ref-erence to its relative historical genesis from prior realistic and rational representations. Thisis exactly what the epistemological profile tries to make explicit. Whatever is abandonedfrom the comprehension of the notion due to scientific scrutiny still remains inherent to thenewly evolved notion. In short, for Bachelard the actual notion of the atom is the sum, andnot the result, of the scientific criticism based on its first intuitive images. These primary
imaginings are very important, because they serve science as an originator which is intendedto be eradicated but which one ultimately never succeeds in doing. In this regard Bachelardemphasizes the atom model of Bohr as a very good representative of its kind. Scientificallyspeaking, almost nothing remained from the original picture, and its dissolution necessitatedso many no’s that scientific knowledge about the atom made huge progress. It is importantto note that these initial intuitive images are of course not primary in a strong sense, i.e.metaphysically given or universals. They should only be assumed as being initial in theweak sense that they are only a relative starting point depending on the currently prevailingscientific mind. This already becomes obvious in the example stated here. The Bohr modelof the atom is an initial intuitive image bound to a certain era and a certain community. Inthe past the notion of the atom and hence the epistemological profile has certainly factored
62
5.3 Characteristics
in other naive realistic and rationalist images than the Bohr model. Accordingly the notionof the atom will certainly refer to (new) intuitive images due to the progress of science andof the scientific mind in the future.
However, in this day and age the notion of the atom has undergone the very conceptualizationdepicted so far. This can also easily be seen in how the notion of the atom is taught. TheBohr model is still the earliest starting point for introducing somebody to what is knownabout atoms. In this regard the educational process is thus a replication of the historicalprocess of conceptualization.
Bachelard has put forward a fairly plausible example regarding the notion of the atom. Howabout the notion of quantum entanglement? What would the initial intuitive image be in thatcase? Is it possible to reconstruct it in accordance to the Philosophy of the No of Bachelard?What are the difficulties in doing so? And what is the difference compared to the notion ofthe atom?
From all what has been said so far, it should be easy to identify the initial image that is thestarting point of the notion of quantum entanglement. Indeed it is remarkable that it is theabsolute starting point for this notion; there was nothing beforehand. Although the namingfollowed shortly afterwards by Schrödinger (Schrödinger 1935), it has to be rememberedthat devising the notion was a response to Einstein et al. (EPR 1935). Therefore it is apt toassume the EPR thought experiment as the actual underlying image of the notion of quantumentanglement.
Therefore the first to apply something like a no to Einstein’s comprehension of the matterwas Schrödinger. Besides being the first no, it was also the essential one, because it reversedthe entire reasoning of the thought experiment. As we already know, Einstein et al. con-cluded that the theory of quantum mechanics is incomplete on the basis of the fundamentalassumption that objects have property values independent of their observation and the im-possibility of ‘spooky action-at-a-distance’. Schrödinger, however, starts out by assumingthat the theory of quantum mechanics is complete and thus concludes that the assumptionsembraced by Einstein et al. cannot be upheld.
Based on this, we can certainly identify a major difference compared to the image of Bohr’smodel in the notion of the atom. As already stated, Bachelard depicts the progressive dis-mantling of the initial intuitive image by scientific criticism; i.e. saying no to the details theimage implies if taken too literally. This is not the case with quantum entanglement. Onthe contrary, the first step of progression in the conceptualization of quantum entanglementis already the complete reversal of the proposition implied by the starting point. This very
63
5 Counter-Intuitiveness
situation has been incorporated into the previously devised epistemological profile of thenotion of quantum entanglement by assuming negative values for the naive realistic (1) andthe classical rationalistic (3) perspective (see figure 5.3).
Consequently a distinction can be drawn on the basis of the relation of the conceptualizationtowards its initial intuitive image. This difference also characterizes the grade of counter-intuitiveness inherent in the notion. At first sight both scientific notions, that of the atomand that of quantum entanglement, are counter-intuitive in relation to normal everyday lifeexperience. However, taking a closer look shows that they are distinguishable in this matterexactly because of the differing status of their initial images.
The notion of the atom is counterintuitive because the initial intuitive image is refined bya succession of critiques, whereby each of these steps is counterintuitive in relation to theinitial intuitive image. This means that in the case of the notion of the atom the counter-intuitiveness is the sum of counterintuitive refinements employed on the initial intuitiveimage. It is important to note that the relation to the initial intuitive image prevails in apositive way. Although almost completely altered by the criticism, it is possible to back-track and hence reproduce a positive connection to the naive realistic aspects of the notionof the atom.
In contrast, the initial image of the notion of quantum entanglement is somewhat counterin-tuitive all along. The starting point of the notion is already a radical challenge to physicallyvery intuitive assumptions34 which are fundamental to our common comprehension of theworld. A cue that the counter-intuitiveness of quantum entanglement enters right at the be-ginning comes from Schrödinger himself. He devised the notion of quantum entanglement,and in the very same paper also the thought experiment of Schrödinger’s cat (Schrödinger1935, p.812, vol.48). The latter is the radical upscaling of the consequences of quantumentanglement to human dimensions. Thus Schrödinger vividly expressed the fundamentalcounter-intuitiveness of his findings right away.
This means that the counter-intuitiveness of quantum entanglement is already constitutiveof the initial image of the notion and not so much a matter of its refinements. We couldpractically speak of an initial counterintuitive image as the starting point of the conceptual-ization of quantum entanglement. It can thus be deemed impossible to reconstruct a positiveconnection to any naive realistic or classical rationalistic aspects.
The fact that quantum mechanics, and with it quantum entanglement, is backed by numer-ous experiments is of no great relevance here. For example, the experiments of quantum34 E.g. objects are bearers of distinct property values independent of their observation and there is no superlu-
minal influence between distant physical objects.
64
5.3 Characteristics
opto-mechanics try to establish quantum effects at human-size scales. They offer a sortof relationship to the everyday world, because the experiments mostly rely on classical in-struments and concepts in order to realize quantum entanglement. We may recall the basicphysical concepts put forward earlier in this thesis, such as two opposing mirrors making upa cavity, the radiation pressure of light and so on35. None of them are very counterintuitiveper se. However, there is a regime where all of this classical set-up realizes data which isonly comprehensible in terms of quantum entanglement. This passage seems impossibleto comprehend solely by empirical means and without recourse to a positive intuitive im-age. Of course these considerations were also taken into account in the previously devisedepistemological profile of the notion of quantum entanglement (see again (2) in figure 5.3).
Conclusion
We were able to study the specifics of the counter-intuitiveness of the notion of quantumentanglement by employing parts of Bachlard’s epistemological framework and examples.Following Bachelard’s main thought that the comprehension of a notion is comprised ofa spectrum of philosophical perspectives allowed me to generally illustrate the rooting ofcounter-intuitiveness in the very notion. The specific differences between quantum entan-glement and, for instance, the classical notion of mass were shown by producing an epis-temological profile of quantum entanglement. As a result, the notion of quantum entangle-ment revealed a repugnancy in its relationship to the naive realistic and classical rationalisticaspects. More specifically, a distinct counter-intuitiveness for the notion of quantum entan-glement has been identified by also considering the historical genesis of conceptualizationbased on Bachelard’s Philosophy of the No. Namely a counter-intuitiveness that alreadyemerges in the initial image, the originator of a conceptualization. In other words, instead ofan initial intuitive image underlying the comprehension of a notion, such as with commonnotions, an initial counterintuitive image is constitutive of the comprehension of the notionof quantum entanglement.
The path which has led us to these conclusions has been pursued in the light of a weaktype of Copenhagen interpretation, and we will continue to follow it. As has been repeat-edly mentioned, other interpretations such as Bohm’s mechanics, Many Worlds and so on,are not within the scope of this thesis. Therefore it must remain open, whether reasoningbased on different interpretations would have resulted in widely differing conclusions. Inprinciple it should be equally possible to also employ the same instruments, e.g. devising
35 See section 3.2 The Experiments
65
5 Counter-Intuitiveness
an epistemological profile, on all other interpretations; with certainly equally exciting re-sults. The circumstance that strongly speaks for the generality of the conclusions drawnhere is that the as yet unsuccessful search for a proper interpretation of quantum mechan-ics parallels the lack of an initial intuitive image for the notion of quantum entanglement.The sought-after interpretation would have to lessen the contradicting aspects of the currentcomprehension of the matter. In this way it would also automatically supply an initial intu-itive image which would dissolve the counter-intuitiveness of our depiction. The other wayround, if we can somehow come up with an initial intuitive image of quantum entanglement,it would be rather strange to think that a proper interpretation could not easily be found bystraight-forward reasoning.
Of course the hunt for a proper interpretation or an initial intuitive image is one possibil-ity to ease the counter-intuitiveness and the problems in comprehending the subject matter.The alternative, followed up on in the next section, springs from another consideration ofBachelard (Bachelard 1988, p.11). He stresses that our scientific mind, i.e. our reasoningand intuition, is mainly instructed by synthetically produced experience. Hence instead ofsearching for an initial image that fits our scientific mind, it is all about evolving our scien-tific mind in a direction where the counter-intuitiveness of quantum entanglement becomes‘inconceivable’.
66
6 Coping
Until now we have dissected the specifics and highlighted several of the characteristics of thecounter-intuitiveness of quantum entanglement. In the course of doing this, I have assumedand shown that counter-intuitiveness can be understood as an indicator of a problematicsituation; moreover a prominent one.
That raises the following questions: If it is considerable and undesirable, then how shouldwe cope with it? Can we look forward to resolving the situation and improving comprehen-sion of the matter? What are the conceivable prospects? In principle, several scenarios areimaginable; none of them are really exclusive, but nevertheless distinguishable in a broadoutline.
Probably the most wide spread one is the hope for a more viable interpretation of quantummechanics. One which is not smitten with counter-intuitiveness. Such a fitting interpretationmay be found due to some flash of inspiration either based on that which is already known,or led by new discoveries. The following quote is an expression of such an approach:
“As long as there are, how shall I put it, phenomenal equivalent interpretations, I mean those
which obviously do not produce any contradiction to the observations. As long as there are
so many phenomenally equivalent world views, I think our reasoning is still fundamentally
wrong. I really think that there can be only one. Now the question is whether we can learn new
things by experimenting.” 1
– Markus Aspelmeyer, (Interviews 2011g, §70)
The last sentence of the quote was rather a rhetorical question when one considers that quan-tum opto-mechanics, the research field of the experimental group, has the basic intention ofrealizing quantum effects with larger systems. Namely, they plan to stretch the applicabil-ity of quantum entanglement to the limits, other than technical ones, and see what happensthere.2
1 Translated by the author.2 For instance, one of the challenges of the coming years will be to take a closer experimental look at the
relation between quantum physics and gravity (Interviews 2011g, §73).
67
6 Coping
Another scenario is to contest the importance of the problem of counter-intuitiveness. Froma pragmatic point of view, it can be argued that for doing the actual physics it is not impor-tant whether the corresponding theory is intuitively comprehensible or not. What is mainlyvalued with a theory is the power of its mathematical framework and how it enables us topredict and describe the results of the experiments. Quantum mechanics is known to fulfillthese pragmatic criteria very well. A specific variant of this scenario is made explicit in thefollowing quote:
“What entanglement is as such mainly defines itself by what you can do with it, because I
believe nobody really knows what it is. You know a little bit about how to quantify it. How you
can tell if you have got a lot of or a little entanglement. And you ... oh well, you can see the
effects. Sort of teleportation or transmission of information. Simply a resource.” 3
– Jonas Hörsch, (Interviews 2011e, §110)
“And that is entanglement for me. This operational complex. Having said that I cannot say
what it actually is either.” 4
– Jonas Hörsch, (Interviews 2011e, §114)
However, in my opinion the question remains whether such a ‘retreat’ into mere mathemat-ical craftsmanship and an operational understanding of the matter is reasonable in the finalconsequence. With all the opportunities theoretical physics and, more generally, mathemat-ics embodies, well justified by its rise in importance in physics, it must be pointed out thatother vital traits of the discipline of physics also have to be kept in mind. Specifically thetrait which tries to consistently interrelate the knowledge gained with our realm of experi-ence. Bluntly put, physics, in contrast to mere mathematics, is commonly accepted to yieldconceivable explanations – going well beyond operational definitions – about the physicalworld.5 Nonetheless, conceiving quantum entanglement as a resource, like energy, is indeedcommon (Bub 2010).
The third scenario concerns the ability of scientific thinking to progress, adapt and familiar-ize itself with the matter at hand. This means that we might not just rely on ignoring counter-intuitiveness, awaiting new scientific facts or sudden inspiration, but take into account thatour reasoning in that matter is also subject to development and change. The following two
3 Translated by the author.4 Translated by the author.5 For instance, the parameters of statistical thermodynamics are made conceptually comprehensible by in-
terrelating them with the intuitive picture of vast quantities of molecules colliding with each other. In thecontext of the epistemological profile this explanatory effort is connected to utilizing the share of naiverealism (see section 5.3.2 Epistemological Profile of Quantum Entanglement) and stress the historical,pedagogical aspects in order to further comprehension of the matter.
68
statements of an interviewee indicate the possibility of such a change in thinking and inconsequence how the matter is taught:
“This battle between realists and local non-realists is quite fascinating. Because right now it is
becoming hard to find a guy who believes in local hidden variable theories, or even non-local
hidden variable theories. To me personally this looks like people trying to keep the old way of
looking at things; not making the step necessary to understand quantum mechanics.”
– Florian Blaser, (Interviews 2011f, §51)
“Unless there is a big change to quantum mechanics [...], I think the change that might happen
is only at the pedagogical level. People learning differently, having access to more examples.”
– Florian Blaser, (Interviews 2011f, §62)
Particular attention will be paid to the last sentence of this quote, as it motivates the investi-gation of pedagogics6 and technology7 as means of coping with the counter-intuitiveness ofquantum entanglement.
For now, it is important to summarize that these scenarios are neither a complete line-up norexclusive alternatives. In a probable outlook, more or less all of them will play a certainrole: It is very understandable to concentrate on the detailed development and experimentalapplication of the theory, when trying to rationally resolve the counter-intuitiveness of thematter on a general level seems so fruitless; as I have tried to illustrate by this thesis. Thusin the practical work done in this field, it is assumed that scientific facts are to be found inthe future that if not bluntly suggesting a single valid interpretation, at least exclude someof them from the current plethora of possible interpretations. Of course there is more toscience than mere craftsmanship8; for instance its conveyance or its history (pedagogics).Subsequently we have to take into account that science can be conceived as a socio-culturalcomplex, generally disposed to proceed also in its reasoning.9 This implies that in the pro-cess of research, of advancing knowledge and conveying it, not only the comprehension ofthe matter changes, but in the long run also the intuitions about it. Matters which today seemto be counterintuitive are not necessarily immune to being perceived as intuitive when onehas become accustomed to or familiarized with them over time. It is thus conceivable thatthe issue of the counter-intuitiveness of quantum entanglement discussed in today’s contextmay dissipate and become a non-issue in the (near or distant) future. The reasons for thisconjecture will be presented and questioned in the remainder of this chapter.
6 See section 6.3.1 Pedagogics.7 See section 6.3.2 Technology.8 Cf. the philosophical term techne9 See section 6.3 Bachelard: Reason Instructed by Fabricated Experience.
69
6 Coping
6.1 Aim of Science? Coherent System of
Assumptions
Thus far I have established that the counter-intuitiveness of quantum entanglement is prob-lematic in its own right. However, I have not discussed whether this is a relevant matter forthe science of physics. In other words, is there a fundamental need for science to get ridof the incoherences in its assumptions – in our more comprehensive diction referred to ascounter-intuitiveness – or can the science of physics, or even more precise the physicists,live perfectly well with sets of basically contradictory assumptions?
In order to illustrate what could be meant by this, we will take a look at parts of the inter-view conducted with Markus Aspelmeyer. In Interviews 2011g, §50-71 a dialogue unfoldedwhich precisely addresses this topic. The starting point is the widely shared idea10, here inthe words of Aspelmeyer, that the ultimate aim of science is that have all your expectationsshould be consistent with all your observations. This vindicates the assumption of at leastone11 world view which is totally consistent with all our observations. However, in the lightof fundamentally conflicting assumptions visible in the counter-intuitiveness of quantumentanglement, for example, Aspelmeyer is willing to allow for some doubt:
“I think, at least in the empirical sciences, there is the implicit assumption that a world view
[Weltbild] exists which in the end can be carved out. However, I want to underline that this per-
haps must not be the case. So maybe complementarity is something that is also relevant to epis-
temology. Complementarity is something, also in principle, which is applicable to world views
[Weltanschauungen]. That there are different, equivalent descriptions of the world, which are
mutually exclusive because they use complementary notions, but refer to the very same nature,
the very same being [Sein]. That’s a maybe.” 12 13
– Markus Aspelmeyer, (Interviews 2011g, §53)
All in all the general aspiration of the science of physics, put forward here, is to find a worldview which is maximally consistent. Hence it is apt to claim that counter-intuitiveness in
10 Certainly this is only one of many possible conceptions of science and its aims. However, it is the one Ifound with the people interviewed.
11 Multiple to unlimited equivalent world views are also conceivable and not precluded.12 Translated by the author.13 As an aside, it is apposite to suggest that complementarity can easily be comprehended in two different
ways. First it is all about world views being different, even mutually exclusive, but equally capable ofconsistently describing the observable data. On the other hand, the second concerns the situation whereultimately all the observable data cannot be consistently apprehended by one world view, but only bya multitude of mutually exclusive world views. This is a much stronger statement as it precludes thepossibility of a final coherent system of assumptions.
70
6.2 New Generations of Scientists
this field is also an issue for the science of physics in general, as it strives to overcome itin the long run. This is nicely backed by the general tenor that pervaded the interviews.The difficulties in comprehending the matter, i.e. counter-intuitiveness, are not seen as asource of despair but more as a motivation. Almost all of the interviewees stated that theyare challenged by the puzzling features of the matter rather than daunted by them. Forexample see Interviews 2011a, §45 and Interviews 2011f, §51. A more hands-on motive forexperimental work is nicely revealed by the following quote:
“When standing downstairs [in the lab] and optimizing something, this [question about the
comprehension and counter-intuitiveness of quantum mechanics] is of course not relevant.
There I couldn’t care less. But it is simply my motivation, when I am tinkering around to
obtain the last few percent of AOM [acoustic-optical modulator] efficiency [...].” 14
– Witlef Wieczorek, (Interviews 2011d, §74)
At this point it must again be remarked that this specific orientation towards the larger ques-tions about the comprehension of the matter is probably also owing to the fact that researchon the foundations of quantum physics is a core theme of the quantum institute here inVienna. Hence the validity of this observation is first and foremost local.15
6.2 New Generations of Scientists
Another general conception we can draw on in studying how the issue is coped with is thefollowing: New findings which maybe hard to grasp and their handling need one, two ormore generations of scientists to be taken for granted. Max Planck, a founding father ofquantum physics16, who was himself not very confident with his own findings, mentionedthis idea in his Wissenschaftliche Selbstbiographie, Leipzig 1948. He wrote that new sci-entific truths are not established by convincing their opponents, but by them dying out anda new generation which has been raised and acquainted with the truth taking their place.Another and maybe more fitting reference are the following words by Richard Feynman:
“We always have had a great deal of difficulty in understanding the world view that quantum
mechanics represents. At least I do, because I’m an old enough man that I haven’t got to the
point that this stuff is obvious to me. Okay, I still get nervous with it. And therefore, some of
the younger students ... you know how it always is, every new idea, it takes a generation or
two until it becomes obvious that there’s no real problem. It has not yet become obvious to me
14 Translated by the author.15 Cf. section B Group: Supplementary Notes16 See for instance law of black-body radiation (Compendium 2009, p.39f).
71
6 Coping
that there’s no real problem. I cannot define the real problem, therefore I suspect there’s no
real problem, but I’m not sure there’s no real problem.”
– Richard Feynman, (Feynman 1982, p.471)
This quote is especially telling, because it is eminently vague and hence fertile soil in whichto raise the following three issues:
First of all, we will identify what Feynman is circumscribing as a real problem, includingdoubting its existence, with what in our diction is label with counter-intuitiveness. Indeedit appears to be rash to equate something very specific, such as what I have developed sofar, with something so vague as Feynman puts it. However, this reaffirms the picture advo-cated in this thesis that our study of the counter-intuitiveness of quantum entanglement isone of many possible dedicated instances of the prevalent discomfort with the explanatoryinconsistency of the matter. What Feynman vaguely outlined as a real problem can indeedbe pinpointed, but only in the light of an already specific understanding.
The second element of vagueness in the quote concerns the meaning of ‘generations of sci-entists’ in this context. How long does a generation of physicists last? What is a generation,and especially in the context of quantum physics? Answering these questions adequatelycertainly exceeds the scope of this thesis. Here I will primarily raise such questions. Thedominating concerns are the conflating definitional aspects of the term generation. In gen-eral, generations are separable in a cursory manner based on time constraints. However,these time constraints which separate generations only make sense due to other distinguish-ing features. For instance, a human familial generation can be defined by the average timebetween a mother’s first offspring and her daughter’s first offspring. This implies that notonly the biological, but also all the social circumstances17 of procreation are represented inthe time tag a generation is labeled with. In the context of generations of scientists, thisinvolves not only the reproduction of knowledge, say education, but also for instance thetime it takes new generations of scientists to become influential and efficacious. What areapt criteria for calling the upcoming scientists a new generation? Exaggerating the quote byFeynman illustrates the intricacy of the issue. The general idea is that the comprehension ofa matter changes over the course of one or two generations of scientists. In order to distin-guish between generations, we need criteria which reveal them to be specifically differentfrom others. A simple criterion such as time which has passed is not sufficient. The mostfitting criterion would be that of a fundamental change in the comprehension of the matter
17 E.g. when is it culturally accepted and common to become pregnant. For an introduction to the topic andas example see Denham 2011
72
6.3 Bachelard: Reason Instructed by Fabricated Experience
at stake.18 However, with such a definition of generations it is rather circular to state thatthere is change through successive generations. We can make this even more tangible. Quitesome time has passed since the beginnings of quantum physics, and even Feynman’s quoteis already thirty years old. Have new generations of scientists already emerged in this fieldof research? In terms of the time scale, we might have to say yes. In terms of generationsthat have fundamentally changed their comprehension of the matter, we might be inclinedto generally tend to say no. As shown in this thesis for example, we are able to call the fun-damental questions raised at the beginning of quantum entanglement (EPR, Schrödinger)still valid, relevant and unresolved. Thinking in generations in this matter thus can be veryambiguous if examined in detail, as has just been hinted at.
The third issue which is vague in this quote by Feynman is the mechanism or process inplace which makes generations proceed in their thinking. What is it that makes us assumethat new generations of scientists will cope differently with the questions raised by oldergenerations? It will not just be time passing by. Hence this is again a vast question toelaborate on and can certainly not be dealt with exhaustively within the scope of this thesis.As a consequence I will just take a look at the two already broached aspects of pedagogicsand technology in the following sections.
6.3 Bachelard: Reason Instructed by Fabricated
Experience
Again we will first employ an idea stemming from Gaston Bachlard. He tries to show thatscientific thinking is essentially oriented towards the realization of the rational (Bachelard1988). Thus Bachelard establishes that this type of realization is the unique feature of to-day’s19 scientific thinking, which clearly distinguishes it from the preceding ones. Thisrealization has nothing to do with a traditional philosophical realism. It is a second orderrealism which is a response to a familiar reality and which is in conflict with the immediate.It is a realism based on a realization of reason instructed by produced experience (Bachelard1988, p.10f).
In order to apply this assessment of scientific thinking by Bachelard, we first of all haveto assume that it is still viable for today’s science. It seems very apt to do so, especiallyin the case of quantum physics. Bachelard invoked quantum physics as one of the major
18 In Kuhnean terms we might speak of a change of paradigms.19 Bachelard refers to the science of his days, roughly at the beginning of the twentieth century.
73
6 Coping
examples20 for this shift towards a new scientific spirit. Furthermore, the fundamentalsof quantum physics, which originated at the beginning of the twentieth century, are stillgenerally valid and in place. Hence we can consider Bachelard’s reflections appropriate fortoday. This can also be bolstered by recalling the actual experiments presented in this thesis.
Bachelard calls this second order realism and we can easily obtain an the idea of it in thecase of quantum opto-mechanics. In the beginning there is a rational consideration thatquantum effects, such as quantum entanglement, are theoretically not bound to the size ofthe system they are implemented with. This thought is in conflict with the immediate andfamiliar comprehension of the world; in our diction meaning it is counterintuitive. Hencethe immediate reality is not the subject matter of our knowledge any more. Rather it isthe produced reality and the experience gathered there which amounts to our knowledge inthis case. Therefore experiments have to be conducted in order to create the phenomena.It is important to note that this is done not because it is easier and more reproducible toaccomplish an observation in the laboratory, but the phenomenon simply would not existif it were not produced there. For Bachelard the conditions of the produced experienceare determined by the requirements of the experiment (Bachelard 1988, p.15). Which, asBachelard continues, shifts the emphasis to the technical problems that have to be masteredin order to produce the phenomena. In the case of quantum opto-mechanics, as well as mostother quantum experiments, it is about excluding environmental influences.21 For example,such technical measures are the extreme cooling of the apparatus and its placing in a vacuum.Even more specifically, in the case of the experiments introduced in this thesis, the possibilityto even come close to a realization of quantum effects strongly depends on the mastery of theproduction of these tiny high quality mirrors on a cantilever. Nevertheless, everything whichis done in order to conduct the experiments is done to produce experience. Experience whichagain feeds back and instructs reasoning accordingly. Referring to our case of quantumopto-mechanics, the general idea, aim or hope is that by fabricating quantum effects at evergrowing size scales, new experiences and hence new knowledge22 will be gathered.
In order to better apprehend this fabrication of experience, we will take a closer look at twocentral aspects (pedagogics and technology) of rationally immersing oneself in a manufac-tured experience especially in the case of quantum opt-mechanics.
20 See chapter 4 in Bachelard 1988, p.86-10021 See the concept of decoherence (Bacciagaluppi 2008; Compendium 2009, p.155ff).22 One future scenario is that of reaching a yet unknown border which would hint at a limit to the applicability
of quantum mechanics, or maybe something else as yet unforeseen.
74
6.3 Bachelard: Reason Instructed by Fabricated Experience
6.3.1 Pedagogics
A very important facet in the progression of the comprehension of a matter, such as the me-diation of the counter-intuitiveness of quantum entanglement in our case, is its conveyance.The first things that come to mind are the educational means utilized in the rearing of newgenerations of scientists. However, we should not just confine ourselves to that, becausethere is also conveyance to those who are not future scientists; that is the ordinary people.
The understanding of pedagogics Bachelard advocates throughout his conception of the sci-entific mind is rooted in his epistemology (Bachelard 1980, 1988). The intellectual history ofthe subject matter mainly determines the way its comprehension is imparted. For instance,Bachelard analyzes the passage from Euclidean to non-Euclidean geometry as a rationalleap and not a continuous improvement (Bachelard 1988, p.24ff). The dropping of the Eu-clidean assumption of parallels as lines not intersecting on a plane is not a developmentof Euclidean geometry itself, but due to a fundamental change of thinking. According toBachelard (Bachelard 1988, p.27) it was not the case that mathematicians deeply doubtedthe parallel postulate, but that to a greater degree they attained the freedom to generallyquestion the role parallels on a plane play in Euclidean geometry. In retrospect of course,Euclidean geometry is a nicely deducible special case of non-Euclidean geometry. Hencein contrast to its erratic historical genesis, the chronological latter is prior to the formerin logical terms. Bachelard also analogously exemplifies the transition from Newtonian tonon-Newtonian mechanics (Bachelard 1988, p.45f).
According to Bachelard, the crucial purpose or assignment of the pedagogics in science israther to replicate its historical sequence and convey the change of paradigms than to di-rectly teach the logical order suggested by analyzing the subject matter in retrospect. This isperfectly backed by taking a look at the curriculum of today. Before we learn non-Euclideangeometry, we start out from Euclidean geometry. First we learn Newtonian mechanics be-fore we engage with the theory of relativity. Many other examples could easily be mentionedhere.
That such pedagogics are in place adds up pretty well with the other parts of Bachelard’sepistemology mentioned earlier in this thesis. Take for instance his Philosophy of the No23,building on the idea that our comprehension of a matter is the sum of an initial image andthe rational criticism applied to it. Therefore it is that which is immediately accessible is thestarting point, not only in our conceptualization, but also in our conveyance of the concept toothers. For example, in order to explain or teach someone what an atom is, we most probably
23 See section 5.3.2 Philosophy of the No
75
6 Coping
begin by presenting Bohr’s model of the atom and then inch along the inadequacies of thisstarting point. With that said, it is also apparent that concerning the epistemological profileof a notion, the relativistic and rationalistic fraction are formed in distinction to the precedingnaive realistic and positive empirical fractions.24
The specifics of our actual theme of quantum entanglement with regard to the epistemologi-cal profile and its constitution on a counterintuitive instead of an intuitive image has alreadybeen explicated in section 5.3.2 Conclusion. What is left to ask is whether this particular-ity of comprehending quantum entanglement also manifests itself in the pedagogics of thematter. In essence, Bachelard’s pedagogic of reproducing the relevant historical change inthinking is also applicable in this case. Conveying and teaching the subject matter along thelines of a historical shift in reasoning is basically not impeded by its counter-intuitiveness.However, it adds a relevant degree of difficulty to the pedagogical undertaking.
In fact, the intricacy of the matter seems to be so problematic to convey that in actual physicstraining this Bachelardean approach tends to be rather avoided. The tangible lead which en-titles us to adopt this assertion is the educational vita of the interviewees.25 Across the boardit can be discerned that primary access to the knowledge in this research field normallyproceeds via the teaching of formalism.26 Knowledge concerning the EPR thought experi-ment, for instance, the fundamental considerations of Schrödinger, Bell and so on turns outto be the result of either special personal interest27 or individual professors committed tothis issue28. In this regard, the following story of an interviewee is particularly informative,as extracurricular learning (in summer school) of the historical and the experimental coreaspects led to personal interest in the matter.
“He [Reinhard Werner] had these detectors which somehow clicked subsequently [EPR/Bell
experiment]. And then he also told us about Einstein’s paper [EPR paper]. It certainly doesn’t
happen often that: A) it did not get cited very much at the beginning; almost not at all. And B)
that it took thirty years until there was a relevant answer [Bell inequality]. You could measure
it in an experiment. And that was somehow exciting. The history was exciting, as well as the
problem itself.” 29
– Witlef Wieczorek, (Interviews 2011d, §15)
24 See section 5.3.2 Epistemological Profile25 Again it is important to recall that the data collected only allows claims with local validity.26 For instance see Interviews 2011d, §16-27.27 E.g. see Interviews 2011a, §19 and Interviews 2011f, §6.28 E.g. see Interviews 2011c, §4 and Interviews 2011e, §37.29 Translated by the author.
76
6.3 Bachelard: Reason Instructed by Fabricated Experience
6.3.2 Technology
If we follow Bachelard, merely with his thoughts put forward so far, it becomes clear thattechnology plays a major role in the realization of phenomena. The necessary deploymentof technology determines the actual realization of the phenomena.
The question is how this refers to the overall issue of handling counter-intuitiveness in thismatter. I fleshed out that counter-intuitiveness marks the conflict between everyday lifeexperience and the assumptions necessary for comprehending the phenomenon of quantumentanglement. In principle it is indeed imaginable that one day our everyday life experiencewill be fabricated such as to render familiar the subject matter which is now conceivedas counterintuitive. Of course it is impossible to imagine today what this future everydaylife experience would actually be like. Nevertheless, following Bachelard, instruments arematerialized theories (Bachelard 1988, p.18); as in our case quantum entanglement wouldbe. Hence it would be foreseeable that technology derived from experiments made in thisfield would yield some sort of quantum technology that could find its way into everydaylife. It is not for nothing that the prospect of highly capable appliances (e.g. quantumcryptography or quantum computing) is a driving force in this research area; at least to courtthe funding. Hence what we can hypothetically anticipate is an emergence of technologythat materializes the momentarily counterintuitive theories of quantum mechanics.
Besides such a speculative forecast, it is probably more interesting to study the role of tech-nology in the realm of the scientists engaged in the field. Their working environment, theirmanufactured experience is located in the laboratory. Devising and conducting experimentsis their job. As a consequence it is obvious to assume that if they are engaged with quantumentanglement, they are immersed in all the devices and knowledge applicable to the field.Put differently, if we were to look for a place which would maximally confront us with thepuzzling phenomenal experience of quantum mechanics, like quantum entanglement, wewould have to visit their laboratories.
Nevertheless, immersion in a technological environment where quantum effects are pro-duced does not self-evidently yield a better comprehension of the matter, less struck bycounter-intuitiveness. Let us again make this issue more tangible by referring to the inter-views with the experimenters of the Aspelmeyer group. One of the major questions posedin all the interviews was whether hands-on experimenting helps in becoming accustomed toor appeased with the counter-intuitiveness of the subject matter.
When looking at quantum opto-mechanics we come upon the situation that they are on thebrink of manufacturing quantum phenomena. However, even when fabricating quantum
77
6 Coping
phenomena, they are basically confronted with classical devices in the laboratory.
“At the moment when you stand in front of the experiment you are indeed always dealing with
classical apparatuses.” 30
– Nikolai Kiesel, (Interviews 2011c, §39)
As we have seen in the description of the experiment31, it consists of parts which are veryintelligible in terms of classical physics. The Fabry-Pèrot cavity for example, radiation pres-sure, mirrors on a cantilever and so on. Unfortunately, we also have to bear in mind that thefunctioning of some parts of the set-up are only properly conceivable on the basis of settledquantum physics.32 The lasers deployed or the method of side-band cooling are examplesof such elements. In sum, the experimenters are dealing with an experimental environmentconsisting of instruments which are materialized theories (following Bachelard) of classi-cal physics and quantum physics. The point, however, is that the targeted counterintuitivephenomenon of quantum entanglement is not part of the apparatuses, but rather the resultof bringing them into a distinct state. That means that when the phenomenon has eventu-ally been produced, it will be cognizable by a readout that is classically perceptible, albeitonly interpretable along the lines of quantum mechanics. We need to recall that in essencequantum entanglement is a non-classical correlation of classical measurement results.33 Thesame idea also applies in the quantum opto-mechanical set-up at hand.
For this reason it would seem rather odd to assert that the experimenters are very immersedin a technological environment which actually renders the counter-intuitiveness of the phe-nomena. Hence we should not expect too much familiarization or acquaintance with counter-intuitiveness by means of the present implementation in the experiments. Rather it is apt tothink that the manufacturing of experience is still at an early stage. In addition, althoughstrongly emphasized in this thesis, we should now take a step back from the laboratory anda specific implementation of the phenomenon, and move to the level of the scientific com-munity engaged in this subject matter. There, a growing plethora of varying experimentalset-ups has already been devised to prepare quantum entanglement. On this level it is pal-pable that experience of the phenomenon is manufactured by many diverging instances ofit. We have to keep in mind here, recalling Bachelard, that it is not merely about produc-ing the phenomenon, but about reason being instructed by the experience of the fabricatedphenomenon. A concrete hint on how we might make this intelligible is given by the ex-
30 Translated by the author.31 See section 3.2 The Experiments.32 I.e. quantum physics which is not counterintuitive in the sense put forward in this thesis. For example the
functioning of lasers is well understood in terms of quantum physics and undisputed in its comprehension.33 See section 2.1 Einstein, Podolsky and Rosen.
78
6.3 Bachelard: Reason Instructed by Fabricated Experience
perimenters themselves. It is not so much the specific technological realization which ishelpful in comprehending the subject matter, it is rather the intellectual exchange about therealization of the phenomenon with colleagues and the community which furthers the un-derstanding and the acquaintance with quantum entanglement. For instance, when askedwhether experimenting helps in understanding the matter, Blaser nicely summarizes withhis answer the subtle attitude I encountered among the experimenters interviewed :
“So with this current experiment, no. From the theory I read, the theory papers I read, I get
a bit. I guess I still increase my understanding of the things through interactions with other
people from the quantum group.”
– Florian Blaser, (Interviews 2011f, §58)
79
7 Conclusion
In sum, this thesis, motivated by a common dictum that quantum mechanics is counterin-tuitive and based on a field study of an experimental group, aimed to raise questions aboutthe counter-intuitiveness of quantum entanglement, a key phenomenon in quantum mechan-ics. The notion of counter-intuitiveness put forward here plausibly describes the situationregarding a common comprehension of quantum entanglement. However, this thesis is justa starting point and is far from covering the topic exhaustively. Moreover, it is dependent onthe presumed mainstream interpretation of quantum mechanics. Nonetheless, the notion ofcounter-intuitiveness is apt to generally signify and specify the intricacies of comprehendingquantum entanglement.
The following basic properties of the notion of counter-intuitiveness have been demon-strated:
• Per definition, labeling something as counterintuitive expresses that the matter is not inagreement with the immediate expectations. In the case of the counter-intuitiveness ofquantum entanglement, this conflict touches upon fundamental expectations about theworld we ‘classically’ live in. For example, recall the classical assumption about theproperty values of objects being determined prior to their measurement, or of the localityof events. This high degree of contradiction is well captured by the counter in counter-intuitiveness. It is not that people concerned with the issue do not have intuitions aboutquantum entanglement (= being non-intuitive).1 It is rather the case that the phenomenonof quantum entanglement, already by its definition2, contradicts our classical expectationsmanifested in our everyday lives. This has been specifically made visible by reference tothe actual experiments of the Aspelmeyer group.3
• Besides defining the term counter-intuitiveness, it is also appropriate to analyze someof the more apparent characteristics of the counter-intuitiveness of quantum entangle-ment. This has been accomplished in two steps. First, by comparison with the inevitabil-
1 See section 5.1 General Definition2 See section 2.2 Schrödinger’s Definition of Entanglement3 See section 5.2 Specifics
81
7 Conclusion
ity of perceptual intuitions (Müller-Lyer illusion) and with the counter-intuitiveness ofdeeply classical-physics matters, such as free fall.4 The former indicated that the counter-intuitiveness of quantum entanglement can be described as prevailing despite counter-vailing beliefs, such as perceptual intuitions. The latter illustrated that the counter-intuitiveness of quantum entanglement is more fundamental and less reconcilable withcommon assumptions held about the world than classical – and nevertheless also – coun-terintuitive concepts. Second, this account of the fundamental counter-intuitiveness ofquantum entanglement has been refined by locating the counter-intuitiveness in the com-prehension of the very term quantum entanglement. I devised an epistemological profileof quantum entanglement in order to demonstrate the intricacy at the level of conceptual-ization5. In order to reflect the counter-intuitiveness within the epistemological profile, Icontrived the contribution of a naive realistic and of a Newtonian or Kantian rationalisticunderstanding of quantum entanglement to be negative. With regard to the naive realism,it is assumed negative because there is nothing in daily life which brings about an intu-itive comprehension of quantum entanglement. In the case of the Newtonian or Kantianrationalism, the negative value is owing to the elementary contradiction between classi-cal assumptions of physics, for instance depicted by Einstein’s et al. understanding of theEPR thought experiment and the fundamentals of quantum entanglement.6 Furthermore,I exemplified this difference in conceptualization between the notion of quantum entan-glement and other scientific notions7 by utilizing Bachelard’s Philosophy of the No. Asa result, quantum entanglement, in contrast to other scientific notions, is outlined by thelack of an intuitive initial image upon which refining criticism (saying a justified no tothe initial image) could be based. The conceptualization of quantum entanglement couldbe apprehended as resting on an initial image which is already counterintuitive and hencelocates the counter-intuitiveness of quantum entanglement at this very fundamental levelof comprehension.
In virtue of this, admittedly non-exhaustive, account of counter-intuitiveness and its char-acteristics with regard to quantum entanglement, it is apposite to actually call quantum en-tanglement counterintuitive. With that said, the second issue of interest was just around thecorner, namely analyzing the coping of this counter-intuitiveness. The starting point wasthe question whether the counterintuitive understanding of quantum entanglement is easedby hands-on experimenting. The answers given by the interviewees backed the following
4 See section 5.3.1 By Comparison5 See figure 5.36 See section 2.3 Interim Conclusion 17 Cf. figure 5.2 and figure 5.3
82
assertions:
• Before studying how the counter-intuitiveness of quantum entanglement is coped with,I established that this is a relevant issue. Namely, under the assumption that empiricalscience aims at the consistency of all our expectations with all our observations (i.e.classical and quantum), it is apt to claim that there is a basic aspiration to overcome aspresented here.8
• In order to lead to the question at hand, I differentiated three possible attitudes towardsthe handling of counter-intuitiveness. None of them is actually exclusive, but nonethe-less distinguishable. The first is the longing for a conclusive interpretation of quantummechanics which is not burdened with a counter-intuitiveness which is as fundamentalas propagated in this thesis. The means to accomplish this task are flashes of inspirationconcerning the already known or new discoveries. Secondly, one can also adopt a moreagnostic attitude with respect to the severity of the counter-intuitiveness; for instance astrictly operational definition of quantum entanglement.9 The third and pivotal consid-eration linked to the initial question is based on the idea that reason is able to progress,adapt and familiarize itself with the matter at issue. Hence subject matters which arecounter-intuitive today might become more intuitive in the future due to familiarization.How this applies and which issues could be raised with regard to quantum entanglementhas been shown by the following:
• A central figure of thought in the concept of getting used to initially counterintuitivematters is often associated with the succession of generations of scientists. I gave nodetailed analysis in this regard, but addressed an essential question or issue. If we ascribeupcoming generations with a more casual, or let us say intuitive comprehension of matterswhich have puzzled older generations, we need to come up with criteria for this change incomprehension other than time passing by.10 The obvious one of making new discoverieshas already been mentioned (see last point). The one I pursued in detail is rests uponBachelard’s rationalism that reason can be instructed by fabricated experience.11
• This second order realism according to Bachelard, i.e. actively producing the phenomenato be experienced and thus instructing reason, has been revealed to be a good repre-sentation of the situation of experimental research in this field. Quantum entanglementis far from being passively observable and is actually only realized by the experiment.
8 See section 6.1 Aim of Science? Coherent System of Assumptions9 Cf. quantum entanglement as resource. (Bub 2010)
10 See section 6.2 New Generations of Scientists11 See section 6.3 Bachelard: Reason Instructed by Fabricated Experience
83
7 Conclusion
Therefore at first glance it seemed that quantum entanglement is a candidate suited toinstructing reason by experimenting with the phenomenon. However, having had a lookat two tangible means of experience which bring about the instruction of reason, namelypedagogics and technology, there is a catch to it in the case of quantum entanglement:
– Again I followed Bachelard and conceived pedagogics as being analogue to the in-tellectual history of the subject matter. In other words, pedagogics in science tendsto replicate the historical sequence and conveys the corresponding changes in reasonrather than establishing a sequence of learning which is logical to the subject matter.For instance, Euclidean geometry is usually taught before non-Euclidean geometry,although the former is just a special case of the latter. The reason being that Euclideangeometry is more initial, more immediate relatable to the world we live in. In thisregard, pedagogics is also associated with the Philosophy of the No. In this concept ofBachelard, an initial image of the matter, which conceivability is the prime criteria, isthe starting point for a critical differentiation of the comprehension of the matter. Con-cerning quantum entanglement, the catch is that we cannot make out such an initialintuitive image, but are straight away confronted with the counter-intuitiveness of thematter.12 Hence the pedagogics of quantum entanglement deviates from the given ex-amples and might demand specific deliberations. Elaborating on those was not withinthe scope of this thesis, which humbly restricted itself to raising the issue.13
– The second means of experience which can be deemed instructive for reason is im-mersion into a technological environment which realizes and applies the phenomenon.The people the most in touch with the realization of quantum entanglement are scien-tist conducting quantum experiments, like the Aspelmeyer group. Nonetheless, basedon statements by the interviewees and the counterintuitive character of quantum en-tanglement as described, it turned out that intricacies can also be found here. As hasbeen presented, experiments realizing quantum effects comprise of apparatuses whichare comprehensible in terms of classical physics or settled14 quantum physics. Conse-quently the apparatuses do not constitute a quantum world you could immerse yourselfto. Quantum entanglement is cognizable by a readout that is classically perceptible,albeit only interpretable along the lines of quantum mechanics. This of course cor-rupts the idea of significantly instructing reason in relation to quantum entanglement
12 See section 5.3.2 Philosophy of the No13 See section 6.3.1 Pedagogics14 I.e. quantum physics which is not counterintuitive in the sense put forward in this thesis. For instance, a
laser is well understood in terms of quantum physics and undisputed in its comprehension.
84
by dealing with the technology realizing the phenomenon.15
Although major impediments to two central facets of instructing reason by experiencehave been identified in the case of the comprehension of the phenomenon of quantumentanglement, the thesis finishes with an optimistic outlook. A general hint deduciblefrom the interviews is that intellectual exchange with colleagues and the community aboutthe realization of the phenomenon is a furthering factor concerning the understanding ofand the acquaintance with quantum entanglement.16
In conclusion, this thesis has accomplished its goal of starting off a comprehensive notionof quantum entanglement which illustrates its counter-intuitiveness along the line of threeaccounts which have been discerned but not separated. The introduction of the theoreticaland experimental foundations, drawing on the interviews with researchers in the field andthe instrumentalization of key concepts of Bachelard’s philosophy of science, facilitated ahopefully stimulating analysis of the dictum of quantum entanglement being counterintu-itive. The hope for stimulation is certainly plausible, as the thesis raises more issues than itsettles.
15 See section 6.3.2 Technology16 This is certainly an interesting aspect worthy of detailed elaborations.
85
Bibliography
Aspelmeyer Group
2011 Quantum Foundations and Quantum Information on the Nano- and Microscale,Faculty of Physics, University of Vienna, http://aspelmeyer.quantum.at/ (visitedon 11/05/2011).
Aspelmeyer, Markus
2010 “Quantum mechanics: The surf is up”, in Nature, 2010/04/01/print, pp. 685–686,http://dx.doi.org/10.1038/464685a.
Bacciagaluppi, Guido
2008 “The Role of Decoherence in Quantum Mechanics”, in The Stanford Encyclope-
dia of Philosophy, ed. by Edward N. Zalta, Fall 2008, http://plato.stanford.edu/archives/fall2008/entries/qm-decoherence/.
Bachelard, Gaston
1980 Die Philosophie des Nein. Versuch einer Philosophie des neuen wissenschaftlichen
Geistes. (’La philosophie du non’, 1940), Suhrkamp(stw325), Frankfurt/Main.
1988 Der neue wissenschaftliche Geist, (’Le nouvel esprit scientifique’, 1934),Suhrkamp, Frankfurt/Main.
Bell, John S.
1964 “On the Einstein Podolsky Rosen Paradox”, in Physics, vol. 1, pp.195–200.
Bokulich, Alisa and Gregg Jaegger
2010 Philosophy of quantum information and entanglement, Cambridge Univ. Press,Cambridge, XXX, 277 S.–.
Brown, James Robert and Yiftach Fehige
2011 “Thought Experiments”, in The Stanford Encyclopedia of Philosophy, ed. byEdward N. Zalta, Fall 2011, http://plato.stanford.edu/archives/fall2011/entries/thought-experiment/.
87
Bibliography
Bub, Jeffrey
2010 “Quantum Entanglement and Information”, in The Stanford Encyclopedia of Phi-
losophy, ed. by Edward N. Zalta, Winter 2010, http://plato.stanford.edu/archives/win2010/entries/qt-entangle/.
Cern - European Organisation for Nuclear Research
2011 Why the LHC?, http://user.web.cern.ch/public/en/LHC/WhyLHC-en.html (visitedon 11/21/2011).
Compendium of Quantum Physics: Concepts Experiments, History and Philosophy
2009 , ed. by D.M. Greenberger, K. Hentschel, and F. Weinert, Springer.
Denham, Woodrow W
2011 Familial Generations Tutorial, http://www.escholarship.org/uc/item/5m51s6k6(visited on 01/14/2012).
DePaul, Michael R. and William Ramsey
1998 Rethinking Intuition: The Psychology of Intuition and Its Role in Philosophical
Inquiry, Rowman & Littlefield, Savage, Md. [u.a.], XVI, 335 S.–.
Einstein, Albert, Boris Podolsky, and Nathan Rosen
1935 “Can Quantum-Mechanical Description of Physical Reality Be Considered Com-plete?”, in Phys. Rev., 47, 10 (May 1935), pp. 777–780, DOI: 10.1103/PhysRev.47.777.
Encyclopædia Britannica
2011 “Intuition”, in Encyclopædia Britannica. Encyclopædia Britannica Online Aca-
demic Edition, ed. by Encyclopædia Britannica Inc., http://www.britannica.com/EBchecked/topic/292162/intuition (visited on 11/29/2011).
Enzyklopädie Philosophie und Wissenschaftstheorie (EnzyklPhilWiss)
2010 “Intuition”, in Ins - Loc: Enzyklopädie Philosophie und Wissenschaftstheorie, ed.by Jürgen Mittelstraß and Gottfried Gabriel, Metzler, Stuttgart [u.a.], pp. 59–61.
Feynman, Richard
1982 “Simulating physics with computers”, in International Journal of Theoretical
Physics, 21 (6 1982), pp. 467–488, ISSN: 0020-7748, http://dx.doi.org/10.1007/BF02650179.
FoQuS - Foundations and Applications of Quantum Science
2011 , University of Innsbruck, http://www.uibk.ac.at/foqus/ (visited on 09/20/2011).
88
Bibliography
Gerlich, Stefan et al.
2011 “Quantum interference of large organic molecules”, in Nat Commun, 2 (Apr.2011), pp. 263–, http://dx.doi.org/10.1038/ncomms1263.
Gröblacher, Simon
2010 Quantum opto-mechanics with micromirrors: combining nano-mechanics with
quantum optics, PhD thesis, Universität Wien, http://homepage.univie.ac.at/simon.groeblacher/SGroeblacher_Dissertation.pdf.
Gröblacher, Simon et al.
2007 “An experimental test of non-local realism”, in Nature, 446, (Apr. 2007), pp. 871–875, http://arxiv.org/abs/0704.2529.
Illusionism.org
2008 Müller-Lyer Illusion, Illusionism.org, http://www.illusionism.org/shape-distortion/m%FCller-lyer+illusion/ (visited on 10/11/2011).
Interviews
2011a Interview with Dilek Demir, ed. by Reinhard Stanzl, Transcription (see Appendix,p.100: Dilek_110524).
2011b Interview with Dr. Garrett Cole, ed. by Reinhard Stanzl, Transcription (see Ap-pendix, p.105: Garrett_110610).
2011c Interview with Dr. Nikolai Kiesel, ed. by Reinhard Stanzl, Transcription (see Ap-pendix, p.111: Nikolai_110525).
2011d Interview with Dr. Witlef Wieczorek, ed. by Reinhard Stanzl, Transcription (seeAppendix, p.115: Witlef_110510).
2011e Interview with Jonas Hörsch, ed. by Reinhard Stanzl, Transcription (see Appendix,p.121: Jonas_110622).
2011f Interview with Mag. Florian Blaser, ed. by Reinhard Stanzl, Transcription (seeAppendix, p.127: Florian_110525).
2011g Interview with Prof. Dr. Markus Aspelmeyer, ed. by Reinhard Stanzl, Transcription(see Appendix, p.131: Markus_110706).
IQOQI - Institute of Quantum Optics and Quantum Information
2011 , Austrian Academy of Sciences, http://iqoqi.at/ (visited on 09/20/2011).
JAXA Japan Aerospace Exploration Agency
2011 IKAROS Project, http://www.jspec.jaxa.jp/e/activity/ikaros.html (visited on02/08/2011).
89
Bibliography
Kippenberg, T. J. and K. J. Vahala
2008 “Cavity Optomechanics: Back-Action at the Mesoscale”, in Science, 321, 5893,pp. 1172–1176, http://www.sciencemag.org/content/321/5893/1172.full.pdf.
Lebedew, P.
1901 “Untersuchungen über die Druckkräfte des Lichtes”, in Annalen der Physik, 311,pp. 433–458, http://dx.doi.org/10.1002/andp.19013111102.
LIGO - Laser Interferometer Gravitational-Wave Observatory
2011 , http://www.ligo.caltech.edu/ (visited on 03/18/2011).
Mermin, David N.
1985 “Is the moon there when nobody looks? Reality and the quantum theory.”, inPhysics Today (Apr. 1985), pp. 38–47, http://dx.doi.org/10.1063/1.880968.
Merriam-Webster
2011a “counterintuitive”, in Merriam-Webster Learner’s Dictionary, ed. by Merriam-Webster, http://www.learnersdictionary.com/search/counterintuitive (visited on12/16/2011).
2011b “intuition”, in Merriam-Webster Learner’s Dictionary, ed. by Merriam-Webster,http://www.learnersdictionary.com/search/intuition (visited on 12/16/2011).
Nichols, E. F. and G. F. Hull
1903 “The Pressure Due to Radiation. (Second Paper.)”, in Phys. Rev. (Series I), 17 (1July 1903), pp. 26–50, http://link.aps.org/doi/10.1103/PhysRevSeriesI.17.26.
Nickles, Thomas
2011 “Scientific Revolutions”, in The Stanford Encyclopedia of Philosophy, ed. by Ed-ward N. Zalta, Spring 2011.
O’Connor, J.J. and Robertson, E.F.
2009 Giovanni Battista Benedetti, http://www-history.mcs.st-andrews.ac.uk/Biographies/Benedetti.html (visited on 03/09/2012).
Quantum Optics, Quantum Nanophysics, Quantum Information
2007 Entanglement based quantum communication over 144 km, Quantum Optics,Quantum Nanophysics, Quantum Information, http://www.quantum.at/research/quantum-teleportation-communication-entanglement/entangled-photons-over-144-km.html (visited on 10/15/2011).
90
Bibliography
2011a , http://quantum.at/ (visited on 09/20/2011).
2011b Research: Quantum Teleportation & Communication & Entanglement, Fac-ulty of Physics, University of Vienna, http://www.quantum.at/research/quantum-teleportation-communication-entanglement.html (visited on 10/05/2011).
2011c Research: Wave–particle duality of C60 molecules, http://www.quantum.at/research/molecule-interferometry-foundations/wave-particle-duality-of-c60.html(visited on 03/29/2011).
Redner, S.
2005 “Citation Statistics from 110 Years of Physical Review”, in Physics Today, vol. 58,p. 49, http://arxiv.org/abs/physics/0506056v2.
Rorty, Richard
1967 “Intuition”, in Encyclopedia of Philosophy, ed. by Donald M. Borchert, 2nd ed.,2006, Macmillan Reference, Detroit, Mich. [u.a.], vol. 4, pp. 722–732.
Rowe, M. A. et al.
2001 “Experimental violation of a Bell’s inequality with efficient detection”, in Nature,409, 6822 (Feb. 2001), pp. 791–794, ISSN: 0028-0836, http://dx.doi.org/10.1038/35057215.
Scheidl, Thomas
2009 A fundamental test and an application of quantum entanglement, PhD thesis, Uni-versität Wien. Fakultät für Physik, http://othes.univie.ac.at/4739/.
Schrödinger, Erwin
1935 “Die gegenwärtige Situation in der Quantenmechanik”, in Naturwis-
senschaften, 48,49,50, pp. 807–812, 823–828, 844–849, http://dx.doi.org/10.1007/BF01491987.
Skulls in the Stars
2008 Fabry, Perot, and their wonderful interferometer (1897, 1899), http://skullsinthestars.com/2008/10/16/fabry-perot-and-their-wonderful-interferometer-1897-1899/ (visited on 03/11/2011).
Vanner, M. R. et al.
2011 “Pulsed quantum optomechanics”, in Proceedings of the National Academy of Sci-
ences, vol. 108, no. 39, pp. 16182–16187, http://www.pnas.org/content/108/39/16182.full.
91
Bibliography
VCQ - Vienna Center for Quantum Science and Technology
2011 , http://vcq.quantum.at/ (visited on 09/20/2011).
Vitali, D. et al.
2007 “Optomechanical entanglement between a movable mirror and a cavity field”, inPhys. Rev. Lett., 98, http://arxiv.org/abs/quant-ph/0609197.
Weihs, Gregor et al.
1998 “Violation of Bell’s inequality under strict Einstein locality conditions”, inPhys.Rev.Lett., 81, pp. 5039–5043, http://arxiv.org/abs/quant-ph/9810080v1.
92
Appendices
93
A Acknowledgment
First of all I would like to thank the people of the Aspelmeyer group. The openness withwhich they shared their thoughts with me in the course of the interviews was a stimulatingexperience. Their useful statements motivated and structured the issues raised in the thesisand provided it with actual relevance. Moreover, they were really talkative, and thus for me,a total novice at conducting interviews, the perfect counterparts.
I also wish to thank my supervisor Martin Kusch for his continuous support from the firstdraft of the idea to the final thesis. After all, its formation spread over a year and in thistime he constantly assisted me with very proficient and productive feedback which providedguidance without being patronizing. The most salient assessment to make of our cooperationis the circumstance that I not only learned a whole lot, but that I was able to also provideMartin Kusch with some insights; admittedly mostly concerning physics.
In addition, I also want to mention my fellow students who were, like me, among the last tocomplete the expiring diploma programme in philosophy here in Vienna. The last of a dyingbreed confronted with a shared deadline. These aggravations motivated me to start off aninitiative to support one another by practical means and ease some of the (self-)proclaimedmaverick attitude of philosophers. Again, this was something I did for the first time andwhich has turned out to be a horn of plenty for new exciting experiences. I hope it has notonly been a big help for me but also for others. Thanks to those that became engaged.
Finally, I want to thank all the others who had also a share, however small, in the realizationof this thesis. All those who spared a word of encouragement, took interest in the overalltopic and supported me, of course not only intellectually but also in any other ways. I willnot name anyone – I am really bad with names – you know who I mean, so please feelthanked.
95
B Group: Supplementary Notes
Besides the information already stated, the interviews also contain interesting issues andtrivia which are not directly linked to the subject of the thesis. Even so, they are worthmentioning, at least to convey a more detailed picture of the group.
For people working together, whether in science or any other working environment, an im-portant facility for ‘socializing’ is the break room or kitchen. It is common source and spacefor not only satisfying the elementary needs for food and drink, but also for communicationand coordination. Moreover, it is also a place to celebrate accomplishments1 and discusseveryday business and, likely after long working hours and adequate beverages, the morefundamental questions. In the case of the Aspelmeyer group, the kitchen is steeped in his-tory because it is located in the former office of Erwin Schrödinger. Schrödinger’s desk, inthe corner of the kitchen, is not treated like an exhibit, but still serves its designated use fromtime to time.
Although it might seem obvious, it is important to note that the Aspelmeyer group is partof a larger quantum community in Austria and linked up with research groups around theglobe. It is not a task of this thesis to unravel the entire structure of the Austrian quan-tum community2. It is more relevant to remark that the ‘Viennese community’ has a moreor less homogeneous point of view in terms of the interpretation of quantum mechanics;vaguely describable as a Copenhagen-type attitude with an emphasis on information as thedetermining entity. This can be ascribed to two aspects. First, maintaining diversity onthe fundamental issues, like in this case the interpretation of quantum mechanics, within ateam does not foster collaboration on day-to-day details. As a second aspect, the quantumcommunity in Austria is largely influenced and shaped by Zeilinger3 and his scientific suc-cessors. These circumstances are neither unique nor astonishing for a research community,
1 My very first contact with the group was a spontaneous invitation to the appreciation of Demir reaching asignificant milestone in her project.
2 For a starting point see FoQuS 2011; IQOQI 2011; Quantum 2011a; VCQ 2011.3 This is just to name one of the publicly known contemporary contributors to quantum physics in Aus-
tria. Certainly there are many others to name who have had their share in taking the Austrian quantumcommunity to a high stage.
97
B Group: Supplementary Notes
but worth bearing in mind.
Another interesting detail which was mentioned in the interviews was the difference betweenthe physicists working theoretically and those doing experiments. Wieczorek and Hörschremarked that there is quite some gap between the theoretical and the experimental mind-set, or relationship to the object of research. Unsurprisingly they noted that quite sometranslation work is required in the course of collaboration (see Interviews 2011e, §57 andInterviews 2011d, §78).
The next remark tackles the interconnection of different research fields by the implementa-tion of equal fundamental physical tenets. Shortly before I conducted the interviews, someof the group members attended a presentation about the Laser Interferometer Gravitational-Wave Observatory (LIGO 2011). In principle they also deploy a Fabry-Pèrot cavity4, in theircase on a very large scale to measure very minuscule length variations presumably causedby gravitational waves. The mutual fascination relies on the common demand for highlyreflective mirrors, although those of LIGO are several centimeters in diameter and the onesin opto-mechanics just a few micrometers.
A further circumstance to note is that interpretations and their equivalence in describing theempirical phenomenon of quantum entanglement were not part of the standard curriculumof many of the interviewees. This reflects the impression that in general academic train-ing5 there is a mainstream concept of quantum mechanics which utilizes a minimum set ofassumptions of a Copenhagen-type interpretation, enough to bolster formalism, but not somuch as to remain agnostic about the more fundamental, philosophical inferences of theassumptions. Interpretations which further a different formalism, e.g. Bohmian mechan-ics, are a minority program. This is only an impression about academic education in thisfield and not about the actual, personal standpoints of the long-serving physicists driving thequantum community.
4 See section 3.2 The Experiments for details.5 I am well aware that my personal experience and the handful of statements about the academic training
of two to three universities, mostly located in German-speaking countries, do not allow for such a generalassertion. However, it is apt to assume that a scientific community that is strongly interconnected aroundthe globe will arrive at a minimum standard of formalism for practical collaboration; granted local color.Hence standard academic training is geared towards conveying a mainstream understanding of quantummechanics, especially as natural sciences generally tend to carve out one valid school of thought. Examin-ing one implementation of academic training can therefore be sufficient to make more general assertions.
98
C Transcription of Interviews
The following are transcriptions of the interviews with the members of the Aspelmeyergroup. They have been transcribed in the language they were conducted (German or En-glish). Translations have only been made in the course of citations within in the thesis.
99
Dil
ek_1
10524
Inte
rvie
w m
it D
ilek D
em
ir v
om
24
.05
.20
11
Tra
nsc
rib
ed
by
yott
a,
vers
ion
1 o
f 1
10
52
5
An
fan
g,
pers
ön
lich
e D
ate
n,
Au
sbil
du
ng
(no s
peaker)
Sm
all
talk
1.
Rein
hard
Gu
t. I
ch w
ill
am
An
fan
g n
ur
so F
orm
ali
en
wis
sen
.2
.D
ilek D
as
heis
st?
3.
Rein
hard
Ja.
Wie
alt
du
bis
t?4
.D
ilek W
art
e,
wie
alt
ich
bin
? Ic
h b
in 2
2.
5.
Rein
hard
Nu
r ein
fach
...
Ich
weiß
es
eig
en
tlic
h e
h a
uch
all
es,
dass
du
gera
de D
iplo
marb
eit
sch
reib
st u
sw.
Ab
er
dein
akad
em
isch
er
Gra
d i
st h
alt
gera
de v
or
dem
Mag
iste
r. W
as
du
ja h
off
st z
u w
erd
en
.
6.
Dil
ek Ir
gen
dw
an
n e
inm
al.
7.
Dip
lom
arb
eit
Rein
hard
Ab
er
das
heis
st d
u s
chre
ibst
ja h
ier
die
Dip
lom
arb
eit
.8
.D
ilek Ja
. S
ag
en
wir
ein
mal
so e
igen
tlic
h b
in i
ch s
chon
am
Sch
reib
en
. A
ber
ich
mu
ss n
och
was
nach
mess
en
pra
kti
sch
. A
lso i
st e
s so
ein
e Ü
berg
an
gsp
hase
wo m
an
halt
noch
nic
ht
Dip
lom
an
d i
st u
nd
au
ch n
ich
t m
eh
r S
tud
en
t is
t, a
ber
au
ch n
ich
t sc
hon
weit
er
ist,
son
dern
irg
en
dw
o d
azw
isch
en
noch
heru
meie
rt u
nd
dara
uf
hoff
t, d
ass
es
en
dli
ch e
inm
al
zu E
nd
e i
st.
9.
Rein
hard
Das
Th
em
a g
en
au
der
Dip
lom
arb
eit
ist
...?
10
.D
ilek E
s is
t "R
ad
iati
on
Pre
ssu
re E
ffect
s on
Macr
osc
op
ic S
yste
ms"
. A
lso e
igen
tlic
h m
eh
rM
ech
an
ik u
nd
Op
tik.
Als
o b
asi
cs.
Un
d d
as
ein
zig
qu
an
ten
mech
an
isch
e a
n d
em
Gan
zen
ist
eh
er
dan
n d
er
Str
ah
lun
gsd
ruck
eff
ekt
selb
er.
Die
Id
ee d
er
Dip
lom
arb
eit
ist
ein
fach
nu
r ein
sim
ple
s, e
infa
ches
Exp
eri
men
t zu
hab
en
, b
ei
dem
man
Str
ah
lun
gsd
ruck
dem
on
stri
ert
.
11
.
Rein
hard
Als
o d
as
heiß
t es
au
fzu
bau
en
...?
12
.D
ilek E
s h
at
so B
ere
chn
un
gen
geg
eb
en
un
d d
an
n h
at
sich
halt
hera
usg
est
ell
t, d
as
mü
sste
eig
en
tlic
h f
un
kti
on
iere
n.
Un
d m
ein
e A
ufg
ab
e l
ag
dan
n m
eh
r od
er
min
der
dari
n,
dass
ich
da e
in E
xperi
men
t se
lbst
- a
m A
nfa
ng
mit
Hil
fe n
atü
rlic
h -
, ab
er
dan
n a
uch
selb
er
desi
gn
t, a
ufg
eb
au
t u
nd
gem
ess
en
hab
e.
Un
d jetz
t kom
mt
halt
dan
n:
geg
en
En
de m
üss
en
wir
das
Gan
ze a
uch
dan
n n
och
in
terp
reti
ere
n u
nd
13
.
hera
usfi
nd
en
ob
dan
n a
uch
der
vorh
erg
esa
gte
Eff
ekt
[Str
ah
lun
gsd
ruck
] au
chw
irkli
ch g
en
utz
t w
ord
en
ist
.R
ein
hard
Un
d d
as
ist
jetz
t d
an
n s
ozu
sag
en
der
aktu
ell
e S
tress
das
hin
zub
ekom
men
?1
4.
Dil
ek G
en
au
, w
eil
in
Lu
ft h
ab
en
wir
es
mal
au
spro
bie
rt u
nd
da h
at
es
ziem
lich
gu
tg
ep
ass
t. U
nd
nu
r ein
e M
ess
un
g,
da w
are
n w
ir e
in b
isse
rl d
an
eb
en
un
d w
ir w
isse
nn
ich
t w
aru
m d
as
so i
st.
Jetz
t si
nd
wir
halt
im
Vaku
um
. D
as
wir
d n
och
mal
üb
erp
rüft
un
d d
an
n s
chau
en
wir
was
pass
iert
.
15
.
Stu
diu
m u
nd
Zu
gan
g z
ur
QM
Rein
hard
Wie
bis
t d
u e
igen
tlic
h..
. A
lso w
ie i
st d
ein
Hin
terg
run
d v
om
Stu
diu
m h
er?
16
.D
ilek A
ber
was
gen
au
mein
st d
u m
it H
inte
rgru
nd
vom
Stu
diu
m?
17
.R
ein
hard
Ja a
lso w
ir k
en
nen
un
s ja
teil
weis
e v
om
gem
ein
sam
en
Stu
diu
m.
Als
o n
eh
me i
ch a
n,
dass
du
hie
r in
Wie
n s
tud
iert
hast
. D
u h
ast
als
o h
ier
beg
on
nen
?1
8.
Dil
ek Ja
mit
Nu
ll W
isse
n a
n d
ie P
hys
ik h
era
ng
em
ach
t. A
lso i
ch h
ab
e g
ar
kein
Wis
sen
geh
ab
t, w
as
ja n
orm
al
bei
den
Ph
ysik
ern
nic
ht
so i
st. D
en
n a
lle a
nd
ern
die
beg
inn
en
sin
d i
rgen
dw
ie s
chon
von
An
fan
g a
n O
lym
pio
nik
en
[z.
B.
Ph
ysik
-O
lym
pia
de]
un
d w
as
weiß
ich
nic
ht
noch
all
es.
Das
war
halt
bei
mir
nic
ht
der
Fall
.D
as
heiß
t ic
h h
ab
e n
och
nie
in
mein
em
Leb
en
zu
vor
Qu
an
ten
mech
an
ik g
eh
ört
. U
nd
wie
ich
dan
n z
ur
Qu
an
tem
ech
an
ik g
ekom
men
bin
war
dan
n w
eil
es
mic
h e
infa
chin
tere
ssie
rt h
at.
Das
war
so e
in p
ap
er,
dass
ich
gele
sen
hab
e u
nd
da k
am
EP
R,
EP
R?,
vor
un
d d
an
n h
ab
e i
ch m
ich
gefr
ag
t n
a w
as
ist
den
n d
as.
Un
d d
an
n h
ab
e i
chh
alt
vers
chie
den
e B
üch
er
darü
ber
gele
sen
. Ja
, d
esw
eg
en
.
19
.
Rein
hard
Ok.
Ab
er
das
war
dan
n s
ozu
sag
en
im
Zu
ge v
om
Stu
diu
m?
20
.D
ilek E
s w
ar
eh
er
Fre
izeit
. E
s w
ar
dan
n e
in p
aar
Sem
est
er
lan
g s
og
ar
so,
dass
ich
mein
eS
ach
en
die
ich
eig
en
tlic
h m
ach
en
mu
sste
zu
rück
gest
au
cht
hab
e u
nd
dan
n m
eh
rF
reiz
eit
, u
nte
r A
nfü
hru
ng
szeic
hen
, g
en
om
men
hab
e u
nd
dan
nq
uan
ten
mech
an
isch
e S
ach
en
gele
sen
hab
e.
Au
ch w
en
n s
ie h
alt
zu
hoch
ware
n.
21
.
Rein
hard
Un
d w
an
n w
ar
das
un
gefä
hr?
Zeit
lich
jetz
t im
Stu
diu
m?
Wen
n m
an
jetz
t sa
gt,
dass
die
T2
Vorl
esu
ng
[Vorl
esu
ng
üb
er
die
Th
eori
e d
er
Qu
an
ten
mech
an
ik,
viert
es
Sem
est
er
im D
iplo
mst
ud
ien
pla
n]
das
Ers
te i
st w
o e
s q
uan
ten
mech
an
isch
losg
eh
t.
22
.
Dil
ek S
o r
ich
tig
th
eore
tisc
h i
st e
s n
atü
rlic
h b
ei
der
Qu
an
ten
mech
an
ikvo
rlesu
ng
losg
eg
an
gen
. A
ber
vorh
er
hab
e i
ch a
uch
sch
on
vers
uch
t w
as
mir
selb
stb
eiz
ub
rin
gen
. A
uch
wen
n e
s n
och
nic
ht
gan
z th
eore
tisc
h g
ew
ese
n i
st.
Das
war
soab
dem
zw
eit
en
Sem
est
er.
Als
o a
b d
er
Pri
nzi
pie
n-V
orl
esu
ng
[P
rin
zip
ien
der
Mod
ern
en
Ph
ysik
(S
pezi
ell
e R
ela
tivi
täts
theori
e u
nd
Ele
men
tare
Qu
an
ten
mech
an
ik),
gro
be Ü
berb
lick
svorl
esu
ng
, zw
eit
es
Sem
est
er
imD
iplo
mst
ud
ien
pla
n]
eig
en
tlic
h.
Davo
r h
ab
e i
ch d
en
Arn
dt
[Mark
us
Arn
dt,
leit
et
die
Fors
chu
ng
sgru
pp
e d
er
Mate
riew
ell
en
(W
ell
e-T
eil
chen
Du
ali
smu
s)]
in d
er
Op
tik
[Vorl
esu
ng
] b
esu
cht
un
d d
er
hat
dan
n i
mm
er
gesa
gt
geh
en
sie
halt
zu
den
Vort
räg
en
. U
nd
dan
n w
ar
es
dan
n e
her
so,
dass
ich
die
lan
gw
eil
ige P
rin
zip
ien
-Vorl
esu
ng
- d
ie h
at
der
Bau
mg
art
ner
[Bern
hard
Bau
mg
art
ner]
zie
mli
ch l
an
gw
eil
ig
23
.
C Transcription of Interviews
100
geh
alt
en
- g
ela
ssen
hab
e u
nd
zu
die
sen
Mon
tag
s-Vorl
esu
ng
en
im
mer
geg
an
gen
bin
. A
b u
nd
zu
halt
. U
nd
das
hat
zirk
a a
b d
em
zw
eit
en
Sem
est
er
eig
en
tlic
hb
eg
on
nen
.R
ein
hard
Un
d d
as
hat
dic
h z
ur
Qu
an
ten
mech
an
ik u
nd
zu
den
Leu
ten
geb
rach
t?2
4.
Dil
ek Ja
. W
itzi
gerw
eis
e w
en
n i
ch m
ich
so z
urü
ck e
rin
nere
, w
are
n d
ie L
eu
te d
ie d
an
n i
nd
iese
n M
on
tag
svorl
esu
ng
en
gew
ese
n s
ind
, d
ie s
ind
jetz
t all
e d
a i
n d
er
Gru
pp
e.
Als
o d
er
Mark
us
[Mark
us
Asp
elm
eye
r] w
ar
dan
n o
ftm
als
der,
der
dan
n v
orn
eg
est
an
den
ist
un
d i
rgen
dw
as
gere
det
hat.
Als
o i
ch b
in d
a i
m n
ach
hin
ein
dan
nd
ara
ufg
ekom
men
, d
ass
er
die
org
an
isie
rt h
at.
Ein
paar
halt
von
der
Gru
pp
e s
ind
au
ch d
rin
gese
ssen
, ab
er
ich
hab
e d
ie n
atü
rlic
h d
am
als
noch
nic
ht
gekan
nt.
25
.
Pers
pekti
ve
Rein
hard
Ste
llst
du
dir
vor
dan
n i
n d
em
Feld
zu
ble
iben
, od
er?
So e
ine P
ers
pekti
ve n
ach
der
Dip
lom
arb
eit
?2
6.
Dil
ek A
h,
das.
Ja,
ich
weiß
nic
ht,
ich
fin
de e
s re
cht
inte
ress
an
t. I
ch g
lau
be a
uch
, d
ass
in
kom
men
der
Zu
ku
nft
wir
d d
as
halt
ein
...
Als
o m
an
kan
n s
ich
er
Qu
an
ten
mech
an
ikau
ch i
rgen
dw
an
n e
inm
al
so v
erw
en
den
, d
ass
das
jed
er
zuh
au
se s
teh
en
hat
un
dw
as
völl
ig n
orm
ale
s is
t.
27
.
Rein
hard
Ja,
ja.
Man
hat
das
Gefü
hl,
dass
es
nic
ht
so e
in t
ote
s F
eld
der
Ph
ysik
ist
. Fall
s es
üb
erh
au
pt
so e
twas
gib
t.2
8.
Dil
ek N
ein
, eig
en
tlic
h ü
berh
au
pt
nic
ht.
Ich
gla
ub
e e
s g
era
de d
as
Pro
ble
m,
dass
man
da
noch
vie
l m
ach
en
mu
ss.
Tot
gla
ub
e i
ch i
st e
s n
ich
t. A
lso e
s is
t all
es
an
dere
als
tot.
29
.
Rein
hard
Von
an
dere
n B
ere
ich
en
der
Ph
ysik
, h
at
man
an
dere
Vors
tell
un
gen
, w
as
man
dort
mach
en
kan
n.
30
.
Dil
ek D
u m
ein
st a
uch
ric
hti
g A
nw
en
du
ng
en
? B
ei
mein
er
Dip
lom
arb
eit
, d
a i
st n
ur
seh
rw
en
ig Q
uan
tem
ech
an
ik e
igen
tlic
h d
ab
ei,
bzw
. fa
st g
ar
kein
e, ab
er
mein
Sys
tem
kön
nte
man
lock
er
verw
en
den
als
Sen
sor.
Od
er
kein
e A
hn
un
g,
als
Pow
erm
ess
gerä
t. M
an
mü
sste
es
ein
wen
ig u
mm
od
eli
ere
n,
od
er
als
Dete
kto
r. M
an
kan
n e
s sc
hon
verw
en
den
.
31
.
Au
fgab
e i
m E
xp
eri
men
t /
Roll
e i
n d
er
Gru
pp
e
Rein
hard
Das
bri
ng
t m
ich
dan
n e
igen
tlic
h e
h d
azu
nach
dein
er
Roll
e i
n d
er
Gru
pp
e o
der
imE
xperi
men
t [z
u f
rag
en
]. W
eil
du
sag
st,
dass
ist
ja n
ur
eh
er
so a
m R
an
de
qu
an
ten
mech
an
isch
. T
rotz
dem
ist
es
vom
Pri
nzi
p h
er
Teil
der
ja b
ei
den
an
dere
nE
xperi
men
ten
verw
en
det
wir
d.
32
.
Dil
ek Ja
, d
as
stim
mt.
Weil
eig
en
tlic
h v
erw
en
det
zum
Beis
pie
l d
er
Wit
lef
[Wit
lef
Wie
czore
k,
Beis
pie
lexp
eri
men
t m
ein
er
Dip
lom
arb
eit
] ja
au
ch c
an
tile
vers
un
d d
er
verw
en
det
das
als
cavi
ty.
Un
d e
r kön
nte
eig
en
tlic
h,
un
d s
og
ar
dan
n a
uch
der
Nik
ola
i [N
ikola
i K
iese
l] u
nd
der
Flo
rian
[F
lori
an
Bla
ser]
[beid
e b
eim
Exp
eri
men
tü
ber
die
su
perp
osi
tion
iert
en
Nan
okü
gelc
hen
], d
ie k
ön
nte
n a
uch
ih
re S
yste
me a
ls
33
.
hoch
em
pfi
nd
lich
e S
en
sore
n b
en
utz
en
.R
ein
hard
Das
wäre
dan
n,
wo d
u e
her
so d
ie "
Tis
ch"-
an
wen
du
ng
mach
st.
Es
ist
die
Fra
ge o
bd
ein
es
so e
in D
em
on
stra
tion
ssys
tem
ist
?3
4.
Dil
ek A
lso p
rim
är
ist
es
als
Dem
on
stra
tion
sexp
eri
men
t g
ed
ach
t. D
as
war
au
ch d
er
Gru
nd
waru
m w
ir e
s ü
berh
au
pt
gest
art
et
hab
en
. N
aja
, eig
en
tlic
h g
ab
es
da e
ine
chall
en
ge v
on
den
Op
to-M
ech
an
ikern
un
d d
a w
oll
te d
er
Mark
us
[Mark
us
Asp
elm
eye
r] u
nb
ed
ing
t w
as
hab
en
. U
nd
das
war
eig
en
tlic
h n
ur
ein
Som
merp
roje
kt
un
d h
ätt
e n
iem
als
sow
eit
kom
men
dü
rfen
od
er
soll
en
. U
nd
es
war
natü
rlic
h a
lsD
em
on
stra
tion
spro
jekt
ged
ach
t. E
s g
ab
sch
on
im
Jah
re 1
90
1 E
xperi
men
te d
azu
.
35
.
Rein
hard
Ab
er
es
ist
halt
die
Fra
ge w
ie a
ufw
en
dig
od
er
wie
ein
fach
die
Din
ger
dan
n s
ind
.3
6.
Dil
ek G
en
au
. A
ber
vor
all
em
, ic
h b
eto
ne d
as
au
ch g
ern
, w
eil
das
hab
e i
ch l
etz
ten
s b
eim
DP
G-M
eeti
ng
[D
eu
tsch
e P
hys
ikali
sch
e G
ese
llsc
haft
?] e
rleb
t, w
o d
an
n d
ie L
eu
te z
um
ir g
ekom
men
sin
d u
nd
gesa
gt
hab
en
: "J
ö,
sch
au
ein
Sch
üle
rexp
eri
men
t".
Das
hat
so w
eh
geta
n.
Das
hat
so w
eh
geta
n.
Weil
eig
en
tlic
h k
an
n m
an
au
ch e
ben
zu
mB
eis
pie
l fü
r A
FM
-Can
tile
ver,
als
o d
as
ist
Ato
mic
Forc
e M
icro
scop
y, d
a i
st ja d
as
Pri
nzi
p,
dass
du
so e
inen
can
tile
ver
hast
un
d v
orn
e e
ine S
pit
ze.
Un
d d
an
n f
äh
rst
du
üb
er
die
Pro
be d
rüb
er
un
d m
isst
die
Au
slen
ku
ng
. U
nd
eig
en
tlic
h i
st e
s d
as
selb
e u
nd
kön
nte
st e
s m
it d
em
au
ch m
ach
en
. O
der
halt
noch
sen
isti
ver,
in
dem
du
das
Sys
tem
ein
bis
sch
en
um
mod
eli
ers
t. N
atü
rlic
h m
uss
t d
u A
rbeit
hin
ein
steck
en
,ab
er
es
wäre
mög
lich
.
37
.
Rein
hard
Ab
er
es
ist
halt
sch
on
seh
r g
em
ein
es
als
Sch
üle
rexp
eri
men
t zu
beze
ich
en
.3
8.
Dil
ek A
ber
es
gab
au
ch L
eu
te,
die
zu
mir
gesa
gt
hab
en
: "W
ow
sch
ön
, S
chü
lere
xperi
men
t.D
am
it k
ön
nte
n s
ie v
iel
Geld
mach
en
. G
rün
den
sie
doch
ein
Un
tern
eh
men
". D
as
hab
e i
ch e
ben
au
ch g
eh
ört
.
39
.
Rein
hard
Es
ist
halt
ein
Un
ters
chie
d,
dass
eb
en
au
ch z
u z
eig
en
; w
en
n i
ch s
ag
e i
ch s
tell
e e
ing
an
zes
Lab
or
voll
od
er
ich
hab
e g
en
au
das
gle
ich
e g
eze
igt
mit
vie
l w
en
iger.
40
.
Dil
ek G
en
au
. W
ir h
ab
en
es
sog
ar
Sch
üle
rn g
eze
igt.
Die
fan
den
das
au
ch r
ech
tin
tere
ssan
t. E
s w
äre
eb
en
halt
ein
bis
sch
en
an
stre
ng
en
d w
en
n m
an
sie
gle
ich
vor
ein
en
Gry
ost
ate
n [
"Kü
hls
chra
nk"
in d
em
das
Sys
tem
ru
nte
rgekü
hlt
wir
d u
m d
en
Gru
nd
zust
an
d d
es
Sys
tem
s in
dem
Qu
an
ten
eff
ekte
au
ftre
ten
zu
err
eic
hen
] st
ell
tu
nd
sag
t, d
a m
ach
en
wir
Qu
an
ten
mech
an
ik,
da k
üh
len
wir
ru
nte
r. A
ls w
ie d
iese
skle
ine K
om
pakte
un
d [
wo m
an
leic
ht
zeig
en
kan
n],
da h
ab
en
wir
den
Can
tile
ver,
un
d d
a h
ab
en
wir
den
Lase
rstr
ah
l u
nd
so w
eit
er.
41
.
Rein
hard
Es
ist
dan
n e
h d
ie S
ach
e,
wie
du
dan
n a
uch
die
Sach
en
irg
en
dw
ie d
ars
tell
st o
der
vers
tän
dli
ch m
ach
st.
Weil
du
kan
nst
zw
ar
den
Gry
ost
ate
n z
eig
en
un
d d
ie g
an
zen
Kis
ten
, ab
er
es
ist
halt
sch
on
ein
Un
ters
chie
d o
b i
ch d
as
nach
voll
zieh
en
kan
n.
42
.
Dil
ek Z
ug
eg
eb
en
. F
eyn
man
, d
er
hat
sich
au
ch m
it g
an
z kom
pli
ziert
en
Din
gen
besc
häft
igt,
hat
ab
er
au
ch i
mm
er
wie
der
gesc
hau
t, w
irkli
ch d
ie b
asi
cs [
zum
ach
en
]. E
s als
o r
un
terz
usc
hra
ub
en
un
d d
an
n a
uch
wir
kli
ch e
s ve
rstä
nd
lich
zu
mach
en
.
43
.
Fasz
inati
on
an
der
Qu
an
ten
mech
an
ik
101
Rein
hard
Ob
woh
l d
ein
Exp
eri
men
t n
ur
am
Ran
de m
it Q
uan
ten
mech
an
ik z
utu
n h
at,
was
wü
rdest
du
sag
en
ist
es
was
dic
h i
rgen
dw
ie a
n d
er
Qu
an
ten
mech
an
ik a
nzi
eh
t?O
der
waru
m e
s in
tere
ssan
t is
t fü
r d
ich
Qu
an
ten
mech
an
ik z
u m
ach
en
? W
as
dic
hh
alt
fasz
inie
rt d
ara
n?
44
.
Dil
ek A
lso t
heore
tisc
h fi
nd
e i
ch Q
uan
ten
mech
an
ik z
iem
lich
cool,
weil
irg
en
dw
ie l
äu
ft d
as
bei
mir
etw
as
intu
itiv
ab
. A
lso n
ich
t d
as
ich
, kein
e A
hn
un
g,
der
Best
e i
nQ
uan
tem
ech
an
ik o
der
so w
äre
. W
eil
ich
gla
ub
e s
o e
inen
gib
t es
ein
ers
eit
s n
ich
t,w
eil
nie
man
d e
s so
ric
hti
g v
ers
teh
t, a
nd
ere
rseit
s ab
er.
.. W
as
woll
te i
ch jetz
t sa
gen
?G
en
au
. E
s si
nd
halt
vie
le F
rag
eze
ich
en
in
der
Qu
an
ten
mech
an
ik.
Un
d t
heore
tisc
hg
ese
hen
ist
es
inso
fern
in
tere
ssan
t, w
eil
ein
fach
Sach
en
, d
ie n
orm
al
kla
r si
nd
dan
nn
ich
t m
eh
r kla
r si
nd
. A
lso m
an
mu
ss s
ich
eig
en
tlic
h,
zum
Beip
iel
das
EP
R-E
xperi
men
t, d
as
pap
er
mu
ss m
an
sic
h g
lau
be i
ch z
wan
zig
tau
sen
d m
al
du
rch
lese
n u
nd
man
vers
teh
t es
imm
er
noch
nic
ht.
Weil
im
mer
wie
der
was
dri
n i
st,
was
man
vorh
er
nic
ht
gese
hen
hat.
Un
d d
as
ist
eig
en
tlic
h z
iem
lich
in
tere
ssan
t,fi
nd
e i
ch,
in d
er
Th
eori
e,
dass
man
irg
en
dw
as
fin
det,
was
man
im
mer
wie
der
vers
teh
t. E
s is
t ir
gen
dw
o d
iese
r W
iders
pru
ch:
So s
oll
te e
s eig
en
tlic
h s
ein
, ab
er
die
Qu
an
ten
mech
an
ik s
ag
t es
an
ders
. W
aru
m w
oh
l? U
nd
dan
n k
an
n m
an
darü
ber
grü
beln
. D
as
fin
de i
ch z
iem
lich
cool.
45
.
Un
d e
xperi
men
tell
sin
d h
alt
im
Mom
en
t d
ie E
xperi
men
te,
die
ich
so i
m K
op
f h
ab
e -
als
o w
ir b
esc
häft
igen
un
s ja
mit
cavi
ties
un
d m
it S
pie
geln
- d
as
ist
eig
en
tlic
h v
oll
sch
räg
, w
eil
mein
e c
an
tile
vers
zu
m B
eis
pie
l, d
ie s
ind
sch
on
ric
hti
g m
akro
skop
isch
.U
nd
die
an
dere
n s
ind
au
ch r
ech
t g
roß
. U
nd
wen
n m
an
sic
h jetz
t ü
berl
eg
t, e
s g
ibt
die
s L
IGO
Leu
te [
Lase
r In
terf
ero
mete
r G
ravi
tati
on
al-W
ave
Ob
serv
ato
ry]
am
MIT
[Mass
ach
use
tts
Inst
itu
te o
f Tech
nolo
gy]
, d
ie d
an
n s
o r
ich
tig
mass
ive S
pie
gel
verw
en
den
. A
lso l
etz
ten
s, d
as
war
eh
gest
ern
, w
are
n w
ir b
ei
so e
iner
Kon
fere
nz,
bei
so e
iner
Au
stell
un
g.
Un
d d
a h
ab
en
sie
eb
en
die
se S
pie
gel
au
sgest
ell
t u
nd
die
ware
n s
o g
roß
[ze
igt
mit
den
Hän
den
ein
e A
bst
an
d v
on
~5
0cm
] u
nd
so d
ick [
zeig
tm
it d
en
Hän
den
ein
e D
ick v
on
~1
5cm
]. A
lso d
as
ware
n k
ilog
ram
m-s
chw
ere
Sp
ieg
el.
Un
d jetz
t m
uss
man
mal
vers
teh
en
die
Th
eori
e,
die
man
eig
en
tlic
h n
ich
tso
ric
hti
g g
ut
vers
teh
t, w
ird
um
gese
tzt
au
f ein
e E
xperi
men
t u
nd
das
noch
dazu
so
gro
ß.
Ich
fin
de d
as
cool.
46
.
Rein
hard
Ja,
weil
es
dan
n s
chon
mass
iver
wir
d. D
as
sin
d ja d
an
n s
chon
an
gre
ifb
are
Din
ge.
47
.D
ilek D
as
fin
de i
ch e
ben
zie
mli
ch i
nte
ress
an
t. U
nd
die
Exp
eri
men
te s
ind
halt
seh
r, s
eh
rin
tere
ssan
t, w
as
die
[d
ie L
IGO
Leu
te]
mach
en
.4
8.
Inte
rpre
tati
on
en
Rein
hard
Un
d w
eil
du
das
vorh
er
bei
der
Th
eori
e g
esa
gt
hast
. E
ben
, d
ass
man
sic
h n
ich
tsi
cher
sein
kan
n.
Od
er
eb
en
wie
du
vorh
er
gem
ein
t h
ast
, d
ass
man
sic
h i
mm
er
hin
terf
rag
en
mu
ss u
nd
im
mer
neu
sic
h d
as
üb
erl
eg
en
mu
ss,
je n
ach
Sit
uati
on
. Is
td
a i
rgen
dw
ie r
ele
van
t d
ie I
nte
rpre
tati
on
en
? A
lso w
en
n m
an
jetz
t d
ie n
imm
t d
ie e
sg
ibt,
sozu
sag
en
im
Stu
diu
m z
um
ind
est
ein
mal
hin
gest
ell
t b
ekom
men
hat?
49
.
Dil
ek N
aja
, im
Stu
diu
m g
lau
be i
ch k
rieg
t m
an
ja n
ich
t all
es
au
fgeti
sch
t. E
inig
es
wir
dein
em
nic
ht
erk
lärt
. A
nd
ere
Sach
en
, d
a m
uss
man
gla
ub
e i
ch d
reim
al
irg
en
dw
oh
ing
eh
en
dam
it m
an
ein
mal
an
satz
weis
e e
rklä
rt b
ekom
mt
was
es
zu b
ed
eu
ten
hat
od
er
mal
vers
teh
t.
50
.
Rein
hard
Un
d d
as
ist
halt
die
Fra
ge o
b d
u s
ozu
sag
en
da e
xtra
nach
frag
en
hast
mü
ssen
. O
der
Din
ge h
alt
nic
ht
au
s d
em
Stu
diu
m s
o e
ind
eu
tig
[g
en
an
nt]
word
en
sin
d.
Was
wäre
nd
as
für
Sach
en
, d
ie d
u v
orh
er
gem
ein
t h
ast
?
51
.
Dil
ek Z
um
Beis
pie
l g
ibt
es
ja d
ie K
op
en
hag
en
er
Deu
tun
g,
die
wir
d ja e
inem
eig
en
tlic
h,
ob
woh
l d
ie h
at
au
ch w
ied
er
Form
en
, ab
er
eig
en
tlic
h d
as
All
gem
ein
ste i
st ja d
ieK
op
en
hag
en
er
Deu
tun
g.
52
.
Rein
hard
Die
min
imals
te V
ari
an
te [
der
Kop
neh
ag
en
er
Deu
tun
g]
die
notw
en
dig
ist
um
...
53
.D
ilek D
ie w
ird
ja e
inem
beig
eb
rach
t. A
ber
zum
Beis
pie
l is
t ja
nic
ht
kla
r w
ie d
as
mit
der
Boh
m's
chen
Mech
an
ik i
st.
Un
d d
a w
ar
ich
sog
ar
bei
ein
em
Sem
inar
wo s
ie d
as
sog
en
au
du
rch
gen
om
men
hab
en
. D
a h
at
man
au
ch s
chon
sch
räg
e S
ach
en
geh
ört
. D
aw
ar
es
halt
dan
n s
chw
ieri
g,
dass
was
man
gele
rnt
hat
mit
dem
an
dere
n z
uve
rgle
ich
en
un
d d
an
n i
n V
erb
ind
un
g z
u b
rin
gen
. U
nd
dan
n r
ich
tig
hera
usz
ud
eu
ten
,w
as
ist
jetz
t fa
lsch
, w
as
ist
nic
ht
fals
ch. W
ie h
ab
en
es
die
Ein
en
betr
ach
tet,
wie
hab
en
es
die
An
dere
n b
etr
ach
tet.
Un
d d
as
hat
dan
n f
ür
ziem
lich
vie
lD
isku
ssio
nss
toff
geso
rgt,
wäh
ren
d d
em
Sem
inar.
54
.
Inte
rpre
tati
on
en
/ T
heori
e /
Exp
eri
men
t
Rein
hard
Un
d w
ie w
ürd
est
du
das
verb
ind
en
mit
dem
was
du
jetz
t h
ier
bra
uch
st?
Was
sozu
sag
en
hie
r re
leva
nt
ist?
55
.
Dil
ek Ic
h m
uss
zu
geb
en
ich
bin
ja,
wie
am
An
fan
g g
esa
gt,
zie
mli
ch a
m A
nfa
ng
. U
nd
weil
ich
am
An
fan
g b
in u
nd
weil
das
Stu
diu
m s
elb
er
ziem
lich
th
eore
tisc
h i
st,
mu
ss m
an
ein
mal
exp
eri
men
tell
ein
iges
au
fhole
n.
Als
o i
ch g
lau
be i
ch h
ab
e v
ier
Sem
est
er
lan
gT
heori
e g
eh
ab
t, w
eil
ich
ja n
och
im
Dip
lom
stu
diu
m b
in.
Un
d e
xperi
men
tell
ware
nh
alt
nu
r so
das
An
fän
gerp
rakti
ku
m u
nd
dan
n h
ab
e i
ch n
och
das
Qu
an
ten
op
tikp
rakti
ku
m g
em
ach
t, u
nd
au
ch d
a l
ern
t m
an
nic
ht
wir
kli
ch w
as.
Un
du
m e
hrl
ich
zu
sein
, d
as
was
ich
wäh
ren
d d
em
Stu
diu
m g
ele
rnt
hab
e ü
ber
Qu
an
ten
mech
an
ik,
das
wen
de i
ch jetz
t se
hr
wen
ig b
is e
igen
tlic
h g
ar
nic
ht
an
.
56
.
Nu
r h
alt
wen
n e
s d
aru
m g
eh
t b
ei
an
dere
n E
xperi
men
ten
, w
o e
s m
eh
r u
mQ
uan
ten
mech
an
ik g
eh
t u
nd
wo d
an
n d
isku
tiert
wir
d,
da k
rieg
t m
an
sch
on
ein
iges
mit
un
d e
s g
ibt
au
ch w
ied
er
neu
e S
ach
en
. A
ber
ich
kan
n n
ich
t w
irkli
ch e
twas
imM
om
en
t an
wed
en
, m
uss
ich
zu
geb
en
. Ic
h m
uss
mic
h e
her
dam
it r
um
sch
lag
en
,w
elc
her
Dete
kto
r am
best
en
pass
t u
nd
wie
ich
das
am
gesc
heit
est
en
ju
stie
re u
nd
so w
as.
Das
ist
dan
n w
ied
er.
.. T
heore
tisc
h g
ese
hen
kan
n i
ch s
o g
ut
wie
garn
ich
tsan
wen
den
. U
nd
exp
eri
men
tell
bie
tet
sich
gera
de b
ei
mein
em
Exp
eri
men
t d
as
nic
ht
so g
esc
heit
an
. Ic
h g
lau
be w
en
n m
an
wir
kli
ch d
as
Sta
diu
m e
rreic
ht,
wo m
an
das
an
wen
den
kan
n,
was
man
vor
Jah
ren
in
der
Qu
an
ten
mech
an
ikvo
rlesu
ng
gele
rnt
hat,
dan
n v
erg
eh
en
ein
mal
so e
inig
e J
ah
re.
Es
mu
ss e
inm
al
au
ch e
in E
xperi
men
tse
in,
das
sch
on
sow
eit
ist
, u
nd
dan
n e
rst.
Ab
er
vorh
er
kan
nst
du
es
verg
ess
en
, d
as
kan
nst
du
sp
aß
halb
er
mach
en
.
57
.
Rein
hard
Un
d I
nte
rpre
tati
on
en
, w
ie d
u g
esa
gt
hast
vorh
er
bei
dem
Sem
inar,
sin
d ja d
an
nn
och
weit
er
weg
? F
ür
das
eig
en
tlic
he E
xperi
men
t d
an
n v
iell
eic
ht
noch
wen
iger
rele
van
t?
58
.
Dil
ek Ja
, ic
h g
lau
be s
chon
.5
9.
Rein
hard
C Transcription of Interviews
102
Ab
er
du
wü
rdest
sch
on
sag
en
, d
ass
das
zum
ind
est
als
Dis
ku
ssio
n s
chon
statt
fin
det?
Als
o I
nte
rpre
tati
on
ssach
en
od
er
die
se T
heori
eg
esc
hic
hte
n?
60
.
Dil
ek D
och
sch
on
, w
eil
es
gib
t ja
im
Mom
en
t ein
Exp
eri
men
t -
bald
hoff
en
tlic
h s
ow
eit
ist
- u
nd
da w
ird
es
dan
n,
sob
ald
man
Erg
eb
nis
se h
at,
wie
der
aktu
ell
werd
en
. A
lso i
mS
inn
e v
on
: d
a w
ird
man
sic
h n
och
mal
üb
erl
eg
en
mü
ssen
, w
ie m
an
das
üb
ert
räg
tau
f d
as
Exp
eri
men
t. A
lso w
en
n m
an
die
gan
ze S
ach
e m
it d
em
, kein
e A
hn
un
g,
Tele
port
iere
n o
der
mit
dem
EP
R d
ara
uf
üb
ert
räg
t. D
a b
in i
ch m
ir s
ich
er
wir
d s
eh
rvi
el
dis
ku
tiert
werd
en
. [S
ie s
pri
cht
hie
r vo
n d
er
An
wen
du
ng
op
to-m
ech
an
isch
er
Qu
an
ten
syst
em
e,
wie
sie
in
der
Gru
pp
e e
rfors
cht
werd
en
, fü
r d
ieQ
uan
ten
info
rmati
on
stech
nik
]
61
.
Vers
teh
en
du
rch
Exp
eri
men
te?
Rein
hard
Wie
sie
hst
du
das
in B
ezu
g a
uf
das
Vers
teh
en
? H
elf
en
dir
sozu
sag
en
die
Exp
eri
men
te -
nach
zuvo
llzi
eh
en
od
er
zu v
est
eh
en
-,
hil
ft d
ir d
as
au
ch b
ei
den
grö
ßere
n S
ach
en
?
62
.
Dil
ek W
as
mein
st d
u m
it g
röß
ere
n S
ach
en
?6
3.
Rein
hard
Ja,
wie
jetz
t In
terp
reta
tion
en
od
er
die
th
eore
tisc
hen
Sach
en
od
er
die
EP
RG
esc
hic
hte
n. W
ürd
e e
s h
elf
en
wen
n d
u s
ieh
st w
as
in d
er
Gru
pp
e p
ass
iert
jetz
t m
itd
en
can
tile
ver
Sach
en
un
d d
en
Vers
chän
ku
ng
s S
ach
en
. U
nd
wen
n d
u d
an
nzu
rück
geh
en
wü
rdest
un
d d
ir d
ie E
PR
Sach
en
an
sch
au
st,
hil
ft e
s d
an
n?
64
.
Dil
ek D
as
man
es
bess
er
vers
teh
t? I
ch g
lau
be w
en
n m
an
das
Exp
eri
men
t se
lber
au
fbau
t,d
an
n h
at
man
sch
on
irg
en
dw
ie e
inen
Bezu
g z
u d
em
un
d v
ers
teh
t es
au
ch v
iel
bess
er,
als
wie
wen
n e
s ein
Koll
eg
e m
ach
t u
nd
sag
t ja
ich
hab
e d
as
un
d d
as
Resu
ltat.
Da m
uss
man
dan
n s
ich
er
län
ger
darü
ber
dis
ku
tiere
n a
ls w
en
n m
an
es
selb
er
gem
ach
t h
at.
Un
d o
b e
s d
an
n h
ilft
die
Th
eori
e b
ess
er
zu v
ers
teh
en
? [P
au
se]
Ich
mein
e,
ich
hab
e e
ine Q
uell
e,
es
geh
t in
die
an
dere
Ric
htu
ng
, u
p o
der
dow
n,.
..Ic
h h
ab
e e
s zu
min
dest
gem
ess
en
. D
.h.,
dass
mein
Resu
ltat
der
Th
eori
e e
nts
pri
cht.
65
.
Rein
hard
Ja,
ab
er
wir
d e
s zu
min
dest
etw
as
reale
r? W
en
n m
an
nu
r d
ie T
heori
e h
at,
ist
es
viell
eic
ht
ein
bis
serl
wu
nd
erl
ich
er,
gera
de w
en
n m
an
so K
on
zep
te h
at
wie
Vers
chrä
nku
ng
od
er
so?
66
.
Dil
ek N
ein
, ic
h g
lau
be n
ich
t. I
ch g
lau
be e
s w
ird
im
mer
noch
ein
bis
sch
en
geb
en
, w
o m
an
sich
den
kt:
Waru
m i
st e
s d
en
n s
o.
Waru
m g
era
de s
o u
nd
nic
ht
an
ders
. U
nd
waru
mp
ass
t g
era
de d
ie T
heori
e z
um
Exp
eri
men
t. I
ch g
lau
be d
ie F
rag
e w
ird
es
imm
er
geb
en
.
67
.
Rein
hard
Als
o d
a s
chein
t d
as
Exp
eri
men
t n
ich
t so
arg
weit
er
zu h
elf
en
?6
8.
Dil
ek D
och
sch
on
, w
eil
du
mach
st M
ess
un
gen
un
d d
u k
an
nst
dam
it w
as
mach
en
. A
ber.
..6
9.
Rein
hard
Vom
Vers
tän
dn
is h
er
wir
d e
s im
mer
noch
kom
isch
, m
erk
wü
rdig
od
er
wie
im
mer
man
das
nen
nen
wil
l? A
lso d
as
ist
die
Fra
ge,
wen
n m
an
rü
ckb
lick
en
d a
uf
die
Sach
en
, d
ie p
ap
ers
die
du
gele
sen
hast
usw
., [
sch
au
t],
un
d jetz
t zu
m U
nte
rsch
ied
exp
eri
men
tell
selb
st m
eh
r in
der
Han
d h
at.
Ob
der
Um
gan
g jetz
t etw
as
leic
hte
ris
t?
70
.
Dil
ek W
en
n i
ch a
n m
ein
Exp
eri
men
t d
en
ke,
dan
n i
st e
s b
ei
mein
e E
xperi
men
t sc
hon
so:
Es
gib
t ein
e T
heori
e,
ich
hab
e e
s g
em
ess
en
, es
pass
t g
en
au
mit
der
Th
eori
eü
bere
in.
Un
d d
.h.
ja d
an
n m
uss
es
halt
so s
ein
. A
ber
bei
den
ric
hti
gen
Qu
an
tem
ech
an
ikexp
eri
men
ten
sin
d e
s ja
vie
l g
öß
ere
Exp
eri
men
te m
it v
iel,
vie
lm
eh
r Para
mete
rn u
nd
da m
uss
man
wir
kli
ch s
org
fält
ig s
ein
. W
en
n m
an
ab
er
sorg
fält
ig g
ew
ese
n i
st u
nd
das
rich
tig
gem
ach
t h
at,
mü
sste
n e
igen
tlic
h k
ein
eF
rag
en
off
en
ble
iben
. A
ber
ich
mu
ss z
ug
eb
en
ich
hab
e s
o e
in E
xperi
men
t n
och
nic
ht
geh
ab
t. I
ch h
att
e n
och
nic
ht
die
Mög
lich
keit
sow
as
zu ü
berp
rüfe
n,
desw
eg
en
gla
ub
e i
ch w
äre
jed
e A
uss
ag
e d
ie i
ch jetz
t tr
eff
e n
ich
t g
an
z d
er
Wah
rheit
en
tsp
rech
en
d.
71
.
Rein
hard
Ja,
das
ist
kla
r.7
2.
Dil
ek A
lso z
u B
eg
inn
hab
e i
ch b
ei
mein
em
au
ch n
iem
als
dara
n g
ed
ach
t, d
ass
ein
makro
skop
isch
er
Sp
ieg
el
du
rch
Ph
oto
nen
bew
eg
t w
ird
un
d i
mm
er
noch
ist
die
Fra
ge o
ffen
ob
es
wir
kli
ch s
o i
st.
Im M
om
en
t is
t es
so,
ab
er
es
kan
n s
ich
jed
eM
inu
te ä
nd
ern
.
73
.
Rein
hard
D.h
. ab
er
meh
r zu
exp
eri
men
tiere
n w
ürd
e d
an
n h
elf
en
,zu
min
dest
mit
den
Sach
en
,w
en
n m
an
so w
ill,
heru
mzu
spie
len
?7
4.
Dil
ek N
ein
, d
as
eig
en
tlic
h a
uch
nic
ht.
Weil
irg
en
dw
an
n e
inm
al
ist
es
halt
so.
Man
kan
nfü
nft
au
sen
d m
al
noch
mess
en
, d
ass
ist
dan
n e
infa
ch s
o.
75
.
Rein
hard
Ja,
ab
er
das
du
zu
min
dest
in
ein
er
an
dere
n V
ari
an
te d
ie D
ing
e n
och
mal
[üb
erp
rüfs
t].
76
.
Dil
ek A
lso w
en
n d
as
Erg
eb
nis
im
mer
noch
das
selb
e i
st u
nd
die
Para
mete
r im
mer
noch
gle
ich
sin
d,
od
er
an
näh
ere
nd
gle
ich
, d
an
n w
ird
man
, g
lau
be i
ch,
nic
ht
noch
meh
rd
ran
sp
iele
n,
weil
es
ein
fach
so i
st.
Weil
eb
en
die
Th
eori
e d
an
n m
it d
em
Exp
eri
men
t n
ich
t ü
bere
inst
imm
t, u
nd
vie
lleic
ht
fin
det
man
da e
inen
Wid
ers
pru
ch.
Un
d z
eig
t d
an
n s
og
ar,
dass
die
gan
zen
hu
nd
ert
Jah
re d
ie d
ie P
hys
iker
dara
uf
au
fgew
en
det
hab
en
, n
ur
Sch
wach
sin
n g
ew
ese
n s
ind
. R
ech
t sc
hw
ieri
ge F
rag
eeig
en
tlic
h.
Ich
hab
e a
uch
selb
er
mir
nie
selb
st d
iese
Fra
ge g
est
ell
t.
77
.
Rein
hard
Es
ist
au
ch d
ie F
rag
e o
b s
o e
twas
für
ein
en
selb
st r
ele
van
t is
t. O
der
eig
en
tlic
h e
gal
ist,
weil
es
für
das
Kon
kre
te n
ich
ts a
uss
ag
t od
er
nic
ht
hil
ft.
78
.
Dil
ek A
lso i
m M
om
en
t h
alt
nic
ht.
79
.
Tech
nis
ch
er
Fort
sch
ritt
Rein
hard
Hat
jetz
t eig
en
tlic
h b
ei
dein
em
Exp
eri
men
t d
er
tech
nis
che F
ort
sch
ritt
geh
olf
en
hat?
Od
er
sin
d e
s eig
en
tlic
h S
ach
en
die
es
sch
on
län
ger
gib
t?8
0.
Dil
ek N
aja
. D
ie S
pie
gel
die
jetz
t g
eb
au
t w
ord
en
sin
d,
da i
st e
s sc
hon
die
zw
eit
eG
en
era
tion
an
Sp
ieg
el
die
wir
verw
en
den
. S
o g
ese
hen
...
81
.
Rein
hard
Ja,
weil
du
bra
uch
st z
iem
lich
gu
t re
flekti
ere
nd
e S
pie
gel.
82
.D
ilek
103
Gen
au
. S
eh
r, s
eh
r, s
eh
r, s
eh
r g
ute
Sp
ieg
el
mit
geri
ng
er
Ab
sorp
tion
. O
bw
oh
l ic
hm
ich
wu
nd
ere
, ic
h h
ab
e i
mm
er
noch
meh
r A
bso
rbti
on
, als
die
se f
ett
en
LIG
O [
Lase
rIn
terf
ero
mete
r G
ravi
tati
on
al-W
ave
Ob
serv
ato
ry]
Sp
ieg
el.
Das
war
un
fass
bar,
die
sin
d s
o g
roß
un
d s
o d
ick u
nd
, kein
e A
hn
un
g,
25
Kil
og
ram
m s
chw
er.
Un
d m
ein
s is
tn
ur
nan
og
ram
m-s
chw
er.
Ab
er
die
hab
en
im
mer
noch
wen
iger
Ab
sorp
tion
.
83
.
Un
d e
s g
eh
ört
gla
ub
e i
ch s
chon
au
ch e
in b
issc
hen
Wis
sen
un
d e
ben
ein
e A
rt v
on
Fert
igkeit
dazu
die
se S
pie
gel
au
ch b
au
en
zu
kön
nen
. U
nd
eig
en
tlic
h h
ab
en
es
die
frü
her
19
01
mit
gan
z si
mp
len
, als
o a
uch
mit
gro
ßen
Sp
ieg
eln
gem
ach
t, a
lso a
uch
so M
ikro
skop
spie
geln
, u
nd
sic
h e
ine g
an
z ve
rrü
ckte
Au
fhän
gu
ng
üb
erl
eg
t. U
nd
dan
n h
ab
en
sie
es
halt
gem
ach
t. W
ir h
ab
en
halt
die
kle
inen
Sp
ieg
eln
. Ja
, ic
hg
lau
be w
en
n m
an
die
se d
iele
ktr
isch
en
Sp
ieg
el,
so w
ie s
ie g
eb
au
t w
erd
en
...
Hätt
ees
die
nic
ht
geg
eb
en
, h
ätt
e e
s d
as
Exp
eri
men
t au
ch n
ich
t g
eg
eg
eb
en
. D
ieD
ete
kto
ren
die
ich
verw
en
de s
ind
eig
en
tlic
h,
als
o i
m V
erg
leic
h z
u 1
90
1..
.
84
.
Rein
hard
Ja,
ok.
Ab
er
es
sin
d s
chon
Din
ger,
die
man
ein
fach
bekom
men
kan
n.
Bis
au
f d
ieS
pie
gel,
die
mu
ss m
an
ext
ra h
ers
tell
en
, d
a m
uss
man
Au
fwan
d r
ein
steck
en
, d
en
Rest
nim
mt
man
sozu
sag
en
vom
Reg
al.
85
.
Dil
ek Ja
, d
as
stim
mt.
Es
hat
ja a
uch
vorh
er
die
Sp
ieg
el
geg
eb
en
un
d d
an
n i
st d
ie I
dee
gekom
men
. S
ow
ie H
en
ne o
der
ist
das
Ei
vorh
er
dag
ew
ese
n.
86
.
Rein
hard
D.h
. ab
er
[zu
ers
t] d
ie t
ech
nis
che M
ög
lich
keit
den
Sp
ieg
el
zu h
ab
en
un
d d
an
nsc
hau
e i
ch m
ir a
n,
dass
ich
das
dam
it m
ach
en
kan
n.
87
.
Dil
ek G
en
au
. U
nd
norm
ale
rweis
e w
erd
en
bei
un
sere
n E
xperi
men
ten
, b
is a
uf
beim
Mic
hael
[Mic
hael
Van
ner]
, ve
rwen
den
all
e a
nd
ere
n e
h n
ur.
.. a
lso W
itle
f [W
itle
fW
iecz
ore
k]
zum
Beis
pie
l, s
ein
Sp
ieg
el
ist
nu
r au
f d
er
ein
en
Seit
e h
och
refl
ekti
v,ab
er
au
f d
er
Rü
ckse
ite n
ich
t. U
nd
das
mu
sste
eb
en
bei
mir
sein
. W
eil
ich
von
der
ein
en
Seit
e A
usl
ese
un
d d
as
von
der
an
dere
n S
eit
e a
usl
en
ke.
Dafü
r h
at
Garr
ett
[Garr
ett
Cole
] zi
em
lich
vie
l A
rbeit
sch
on
rein
gest
eck
t, d
am
it e
r ein
mal
hera
usfi
nd
et
wie
man
au
f b
eid
en
Seit
en
das
ed
ged
.
88
.
En
de
Rein
hard
[Pau
se]
Als
o m
ein
e F
rag
en
wäre
n d
am
it e
rsch
öp
ft.
89
.D
ilek P
rüfu
ng
best
an
den
?9
0.
Rein
hard
Es
gib
t kein
e P
rüfu
ng
. A
lso w
en
n,
dan
n b
in i
ch d
er
Prü
flin
g i
n d
iese
r S
itu
ati
on
.9
1.
Wen
n d
u n
och
Fra
gen
hast
?9
2.
(no s
peaker)
Ku
rzes
Gesp
räch
, w
as
so d
er
Ph
iloso
ph
mach
t. D
an
ksa
gu
ng
un
d a
usk
lin
gen
der
small
talk
.9
3.
C Transcription of Interviews
104
Garr
ett
_110610
Inte
rvie
w m
it D
r. G
arr
ett
Cole
vom
10
.06
.20
11
Tra
nsc
rib
ed
by
yott
a,
vers
ion
5 o
f 1
10
61
7
An
fan
g,
pers
ön
lich
e D
ate
n,
Au
sbil
du
ng
(no s
peaker)
[in
tro s
mall
talk
]1
.R
ein
hard
Just
for
a s
tart
, co
uld
you
tell
me y
ou
r ag
e?
2.
Garr
ett
I ju
st t
urn
ed
32
in
May
31
st.
3.
Rein
hard
Th
en
, w
hat
is y
ou
r ed
uca
tion
al
back
gro
un
d?
4.
Garr
ett
Bach
elo
rs d
eg
ree i
n m
ate
rials
en
gin
eeri
ng
. S
o I
'm o
rig
nall
y fr
om
San
Fra
nci
sco
are
a.
Th
en
I w
en
t to
th
is s
chool
in,
you
neve
r h
eard
of,
Cali
forn
ia P
oly
tech
nic
Sta
teU
niv
ers
ity.
It'
s li
ke a
sm
all
poly
tech
nic
sch
ool.
Th
ey
had
a m
ate
rials
en
gin
eeri
ng
for
bach
elo
rs.
An
d t
hen
I w
en
t to
San
ta B
arb
ara
, U
C S
an
ta B
arb
ara
, fo
r, i
t's
just
call
ed
'M
ate
rials
' th
ere
, b
ut
it's
mate
rials
sci
en
ce a
nd
en
gin
eeri
ng
. B
ut
it's
als
o i
nth
e c
oll
eg
e o
f en
gin
eeri
ng
th
ere
. S
o i
t is
con
sid
ere
d a
n e
ng
ineeri
ng
dep
art
men
t.M
ate
rials
is
a v
ery
bro
ad
field
. S
o I
act
uall
y d
id e
lect
ron
ic a
nd
ph
oto
nic
mate
rials
.S
o i
t's
more
ap
pli
ed
con
den
sed
matt
er
stu
ff;
ap
pli
ed
soli
d s
tate
. A
nd
th
ere
I d
id m
yP
hD
in
20
05
. A
nd
th
en
I w
ork
ed
in
in
du
stry
for
a y
ear.
I w
ork
ed
at
Law
ren
ceL
iverm
ore
, it
's a
Nati
on
al
Lab
ora
tory
in
th
e U
S,
for
two y
ears
. A
nd
th
en
here
.L
iverm
ore
is
a b
ig...
So t
here
is
Los
Ala
mos
an
d L
iverm
ore
. S
o L
os
Ala
mos
was
firs
t...
Liv
erm
ore
was
bu
ild
to d
eve
lop
th
e h
ydro
gen
bom
b.
So i
t's
to b
uil
dth
erm
on
ucl
ear
wep
on
s. S
o i
t's
a w
eap
on
s la
b.
Bu
t n
ow
it'
s ju
st a
gen
era
l sc
ien
tifi
cre
searc
h l
ab
.
5.
Werd
eg
an
g
Rein
hard
How
did
you
kin
d o
f tr
an
sfer
from
th
e m
ate
rial
en
gin
eeri
ng
part
to s
om
eth
ing
lik
eh
ere
, th
e p
hys
ics
dep
art
men
t?6
.
Garr
ett
So m
y b
ack
gro
un
d i
s in
mic
ro-n
an
o f
ab
rica
tion
. I
have
a r
eall
y w
eir
d b
ack
gro
un
d.
So e
ven
th
ou
gh
by
deg
ree,
the d
eg
ree m
ate
rial
scie
nce
, m
ost
of
the w
ork
I'v
e d
on
eh
as
been
ju
st a
pp
lied
devi
ce d
esi
gn
an
d f
ab
rica
tion
. F
or
my
dis
sert
ati
on
rese
arc
h I
mad
e d
iod
e l
ase
rs.
So t
hese
mech
an
icall
y tu
neab
le d
iod
e l
ase
rs.
Th
ey
are
th
ese
fun
ny,
very
sp
eci
fic
typ
es
of
surf
ace
am
en
din
g l
ase
rs.
So h
ow
to d
o s
urf
ace
leg
it.
Th
en
I m
ad
e a
sm
all
movi
ng
mir
ror
that
wou
ld c
han
ge t
he c
avi
ty l
en
gth
. A
nd
you
cou
ld t
un
e t
he c
en
ter
of
wave
len
gth
wit
h t
his
devi
ce.
If y
ou
look,
this
is
wh
ere
th
eco
nn
ect
ion
s co
me i
n.
I m
ad
e m
ovi
ng
mir
rors
! B
ut
mu
ch m
ore
com
ple
x, c
au
se y
ou
had
a f
ull
dio
de l
ase
r st
ruct
ure
th
at
you
had
to b
uil
d w
ith
th
is m
ovi
ng
mir
ror.
Asu
spen
ded
mir
ror
that
you
ele
ctro
stati
call
y m
ove
d.
An
d t
hen
I d
id t
hat
con
tin
uou
sly
aft
erw
ard
s. S
o i
n i
nd
ust
ry t
here
is
a c
om
pan
y th
at
act
uall
y li
cen
ced
ap
ate
nt
for
som
e o
f th
e w
ork
th
at
we d
id.
Th
ey
stil
l d
eve
lop
th
ese
devi
ces.
An
d a
tL
iverm
ore
I ju
st d
id s
en
sor
deve
lop
men
t. T
hese
th
ing
s are
reall
y fa
st t
un
eab
lela
sers
; n
arr
ow
lin
ew
idth
, ve
ry f
ast
tu
nin
g.
So f
or
gas
sen
sin
g o
r d
isp
lace
men
t
7.
sen
sin
g.
Th
en
I s
aw
th
is o
pto
-mech
an
ics
work
cam
e u
p.
Act
uall
y in
my
stru
ctu
res,
if y
ou
had
hig
h e
nou
gh
in
tra c
avi
ty p
ow
er,
you
cou
ld s
ee s
tati
c d
isp
lace
men
ts o
fth
e m
irro
r; t
hro
ug
h r
ad
iati
on
pre
ssu
re f
orc
es.
Cau
se t
he c
avi
ty l
en
gth
was
two
mic
ron
s, s
o y
ou
get
mass
ive d
isp
lace
men
ts.
Rein
hard
Alt
hou
gh
you
don
't w
an
t th
em
.8
.G
arr
ett
You
don
't w
an
t th
em
! T
hey
are
act
uall
y b
ad
. T
hey
hu
rt t
he s
tab
ilit
y of
the l
ase
r.B
ut
it w
as
alw
ays
an
in
tere
stin
g s
ort
of
asi
de.
Noth
ing
we w
ou
ld e
ver
pu
bli
sh o
n i
t,b
ut
we u
sed
it
just
to p
lay
aro
un
d.
You
cou
ld c
han
ge t
he c
en
tre o
f w
ave
len
gth
of
the l
ase
r b
y p
utt
ing
en
ou
gh
pow
er
in i
t. A
nd
th
en
on
20
05
th
ere
is
these
firs
tp
ap
ers
com
ing
up
, li
ke p
ara
metr
ic o
scil
lati
on
in
th
ese
devi
ces;
in
op
to-m
ech
an
ical
devi
ces.
So I
alw
ays
kin
d o
f w
atc
hed
it.
Wh
en
I w
as
at
Liv
erm
ore
th
e p
osi
tion
was
reall
y n
ice.
Half
of
the t
ime y
ou
had
to d
o w
ork
for
the l
ab
ora
tory
an
d h
alf
th
e t
ime
you
cou
ld d
o a
nyt
hin
g y
ou
wan
ted
; w
hic
h w
as
aw
eso
me.
I en
ded
up
...
So I
sta
rted
tryi
ng
to g
et
mon
ey
inte
rnall
y to
do t
he w
ork
lik
e w
ith
som
e o
ther
peop
le i
n t
he
lab
ora
tory
an
d i
t n
eve
r g
ot
acc
ep
ted
. I
mean
it
was
an
en
gin
eeri
ng
dep
art
men
tan
d t
he a
lways
wan
ted
ap
pli
cati
on
s an
d u
se.
So i
t w
as
alw
ays
sh
utd
ow
n.
An
d t
hen
at
on
e p
oin
t I
was
act
uall
y ju
st w
rote
in
[??
?] t
o p
eop
le t
o w
ork
. A
nd
I w
as
bore
dan
d s
o I
ju
st t
yped
a m
ess
ag
e t
o M
ark
us
[Asp
elm
eye
r],
wh
o I
'd n
eve
r m
et.
An
d ju
stsa
id:
Ok t
his
is
very
in
tere
stin
g a
nd
I c
an
do m
icro
fab
. H
ere
are
som
e i
deas.
An
dse
nt
it t
o h
im.
9.
Rein
hard
An
d h
ow
you
get
to [
kn
ow
] M
ark
us?
10
.G
arr
ett
I sa
w t
he p
ap
ers
. Ye
s ou
t of
the p
ap
ers
. A
nd
I c
on
tact
ed
th
em
an
d M
ark
us
[Asp
elm
eye
r] w
rote
me b
ack
. A
nd
th
en
for
ab
ou
t a y
ear
from
Liv
erm
ore
I w
ork
ed
wit
h M
ark
us
[Asp
elm
eye
r] l
ike f
or
very
sm
all
sid
e p
roje
cts.
Fab
rica
te s
am
ple
s, s
hip
them
to V
ien
na,
they
wou
ld t
est
th
em
, se
nd
me t
he r
esu
lts,
make n
ew
devi
ces
an
dsh
ip t
hem
back
. S
o t
hat
wen
t on
for
a y
ear.
An
d t
hen
un
fort
un
ate
ly t
he l
ab
ora
tory
had
som
e m
ajo
r fi
nan
cial
pro
ble
ms.
So t
hat'
s a w
hole
lon
g s
tory
. S
o t
hey
laye
d o
fflo
ts o
f p
eop
le.
I w
as
exc
ep
t fr
om
th
e l
ayo
ff.
I co
uld
not
get
fire
d,
bu
t it
was
very
dep
ress
ing
.
11
.
Rein
hard
Th
at'
s a p
oin
t to
ju
mp
off
an
d d
o s
om
eth
ing
diff
ere
nt?
12
.G
arr
ett
It l
ook r
eall
y b
ad
an
d I
did
n't
lik
e t
he w
ay
thin
gs
were
goin
g.
I h
ad
a t
alk
to
Mark
us
[Asp
elm
eye
r] a
bou
t it
an
d h
e a
sked
if
I w
an
ted
to c
om
e t
o V
ien
na;
full
tim
e.
So i
t's
a v
ery
lon
g a
nd
com
ple
x co
nn
ect
ion
.
13
.
Rein
hard
Yeah
, b
ut
it i
s kin
d o
f ext
raord
inary
sto
ry,
not
very
com
mon
sto
ry t
o t
ell
.1
4.
Garr
ett
It's
a w
eir
d o
ne.
15
.
ph
ysik
-th
eore
tisc
her
Hin
terg
run
d
Rein
hard
So t
hat
is y
ou
r b
ack
gro
un
d a
lso i
n k
ind
of
ph
ysic
s? T
he t
heory
stu
ff?
16
.G
arr
ett
Th
at'
s ve
ry w
eak.
So c
om
ing
fro
m a
n e
ng
ineeri
ng
back
gro
un
d,
like f
or
my
bach
elo
rs d
eg
ree,
I to
ok a
nu
mb
er
of
soli
d s
tate
cou
rses
an
d a
lots
of
mate
rial
scie
nce
cou
rses.
Bu
t I
took o
ne i
ntr
o..
. It
wasn
't e
ven
qu
an
tum
mech
an
ics,
it
was
17
.
105
mod
ern
ph
ysic
s. S
o i
t h
ad
lik
e r
ela
tivi
ty a
nd
som
e i
ntr
o t
o q
uan
tum
mech
an
ics.
An
d w
hen
I s
tart
ed
gra
du
ate
sch
ool,
I g
uess
I ju
st t
ook t
wo q
uan
tum
mech
an
ics
cou
rses.
So I
took a
gain
som
eth
ing
lik
e a
n i
ntr
o,
bu
t fo
r q
uan
tum
mech
an
ics.
An
dth
en
I t
ook s
om
e,
I d
on
't e
ven
rem
em
ber
the n
am
e,.
.. n
ow
th
is i
s te
n y
ears
ag
o.
Som
e m
ixed
leve
l q
uan
tum
mech
an
ics
cou
rse. I
start
ed
to t
ake a
noth
er
qu
an
tum
mech
an
ics
cou
rse,
act
uall
y th
rou
gh
th
e p
hys
ics
dep
art
men
t. A
nd
I w
as
alr
ead
yd
oin
g r
ese
arc
h a
nd
it
was
just
too m
uch
, so
I s
top
ped
. T
hat
was
it.
Bu
t m
ost
eve
ryth
ing
was
mu
ch m
ore
ap
pli
ed
. A
nd
beca
use
I w
as
in t
his
lik
e e
lect
ron
icm
ate
rials
pro
gra
m..
. S
o y
ou
sort
of
basi
call
y g
ot
the q
uan
tum
iss
ues,
bu
t m
ost
of
itw
as
ap
pli
ed
to l
ike c
on
fin
ed
ele
ctro
nic
str
uct
ure
s.R
ein
hard
Han
dle
d a
s ju
st a
sid
e e
ffect
, w
hic
h y
ou
pro
bab
ly d
on
't w
an
t to
have
?1
8.
Fasz
inati
on
an
der
Qu
an
ten
mech
an
ik
Garr
ett
Yeah
. S
o t
hat
was
inte
rest
ing
. I
mean
it
was
alw
ays
in
tere
stin
g t
o m
e.
Lik
e t
he
'mod
ern
ph
ysic
s' c
ou
rse I
took f
or
my
bach
elo
rs.
I d
idn
't g
et
an
y cr
ed
it f
or
that
class
. It
wasn
't p
art
of
my
curr
icu
lum
, I
just
ad
ded
it
beca
use
I t
hou
gh
t it
was
inte
rest
ing
.
19
.
(no s
peaker)
[lit
tle i
nte
rru
pti
on
]2
0.
Garr
ett
So I
alw
ays
had
an
in
tere
st i
n b
asi
c p
hys
ics.
Th
at'
s on
e o
f th
e r
easo
ns
wh
y I
wou
ldco
me h
ere
. It
wou
ld b
e h
ard
to ju
stif
y co
min
g h
ere
, b
ut
did
n't
lik
e t
he m
ore
fun
dam
en
tal
stu
ff.
21
.
Rein
hard
Th
at
is t
he q
uest
ion
wh
eth
er
you
can
pin
poin
t to
som
ew
here
wh
ere
you
got
start
ed
to b
e i
nte
rest
ed
?2
2.
Garr
ett
No,
it w
as
just
sort
of
alw
ays
th
ere
. I
can
go b
ack
an
d s
ay
som
e w
hole
th
ing
lik
ew
hen
I w
as
you
ng
er.
I l
iked
ast
ron
om
y an
d I
had
som
e [
???]
book t
hat
desc
rib
ed
mod
ern
sci
en
tifi
c st
uff
an
d i
t h
ad
a l
ittl
e d
esc
rip
tion
ab
ou
t th
ing
s li
ke q
uan
tum
mech
an
ics.
So i
t is
alw
ays
in
tere
stin
g.
I'm
su
re e
very
bod
y sa
ys t
he s
am
e t
hin
g,
bu
tju
st t
he c
ou
nte
r-in
tuit
iven
ess
was
inte
rest
ing
to s
om
e d
eg
ree;
rig
ht.
Cau
se t
here
is
som
eth
ing
you
don
't e
xpect
or
don
't s
ee.
23
.
Rein
hard
So t
hat
is o
ne o
f th
e a
ttra
ctio
n p
oin
ts,
esp
eci
all
y in
th
e b
eg
inn
ing
. W
hen
th
ey
com
eu
p w
ith
sta
tem
en
ts t
hat
are
hard
to b
eli
eve
, or
hard
to g
et.
24
.
Garr
ett
Exa
ctly
. It
was
fun
ju
st t
o l
earn
th
e c
on
cep
ts.
25
.
Au
fgab
e i
m E
xp
eri
men
t /
Roll
e i
n d
er
Gru
pp
e
Rein
hard
So w
hat
is y
ou
r cu
rren
t ro
le i
n t
he g
rou
p?
Wh
at
are
you
doin
g?
26
.G
arr
ett
So I
've b
een
here
tw
o a
nd
half
years
now
. I
had
th
is M
ari
e-C
urr
ie f
ell
ow
ship
, w
hic
hw
as
kin
d o
f n
ice.
So m
ain
ly f
or
the g
rou
p I
do l
ike d
esi
gn
th
e r
eso
nato
rs,
mic
rofa
bri
cati
on
of
the r
eso
nato
rs a
t th
e t
ech
nic
al
un
ivers
ity
[Tech
nis
che U
niv
ers
ität
Wie
n].
An
d t
hen
ch
ara
cteri
zati
on
of
the r
eso
nato
rs.
So w
e b
uil
d a
sm
all
test
setu
p..
. C
au
se t
he fi
nal
exp
eri
men
t is
in
th
is d
ilu
tion
fri
dg
e t
hat
takes
days
to c
ool
27
.
dow
n a
nd
it'
s co
mp
lex.
Th
e fi
rst
goal
was
to b
uil
d a
qu
ick t
urn
aro
un
d t
est
ing
syst
em
. S
o i
t w
asn
't t
he f
ull
exp
eri
men
t, b
ut
was
en
ou
gh
to c
hara
cteri
ze t
he
mech
an
ics.
So I
bu
ild
th
is c
ryog
en
ic-e
nab
led
Fab
ry-P
ero
t in
terf
ero
mete
r sy
stem
,w
here
we c
ou
ld l
oad
ch
ips
in, m
easu
re t
he m
ech
an
ical
resp
on
se o
f th
e d
evi
ces
[can
tile
vers
on
th
e c
hip
].It
wasn
't i
nti
all
y th
e p
lan
, b
ut
at
on
e p
oin
t w
e s
tart
ed
gett
ing
...
All
th
ese
th
ing
s are
lim
ited
by
the q
uali
ty f
act
or
of
the r
eso
nan
ce, so
th
e m
ech
an
ical
dam
pin
g o
f th
ere
son
an
ce.
Wh
ich
is
the b
igg
est
road
blo
ck t
o a
ll t
hese
op
to-m
ech
an
ical
exp
eri
men
ts.
So w
e s
tart
ed
lookin
g i
nto
ways
of
qu
an
tifi
ng
an
d u
nd
ers
tan
din
g t
he
mech
an
ical
dam
pin
g i
n t
he s
yste
ms.
28
.
Rein
hard
To i
mp
rove
th
en
on
th
e m
ech
an
ics.
29
.G
arr
ett
So t
hen
I t
ook,
that
was
like t
wo y
ears
alm
ost
, li
ke a
year
an
d a
half
ju
st f
ocu
sin
gon
th
is.
Ult
imate
ly w
e a
lso g
ot
som
e n
ice p
ap
er.
So i
t's
basi
call
y d
esi
gn
, fa
b,
chara
cteri
zati
on
of
the r
eso
nato
rs.
An
d t
hen
th
ere
is
alw
ays
lots
of
litt
le s
ide
thin
gs
that
pop
up
. B
ut
my
main
role
wou
ld b
e t
he g
uy
wh
o w
ork
s in
th
e c
lean
room
.
30
.
Rein
hard
Makin
g a
ll t
his
reso
nato
rs.
An
d t
he o
thers
th
en
sp
oil
th
em
.3
1.
Garr
ett
Ad
ap
t th
em
! T
here
is
Dil
ek [
Dem
ir],
th
is d
iplo
ma s
tud
en
t d
oes
the r
ad
iati
on
pre
ssu
re t
est
wit
h t
hese
can
tile
vers
th
at
I m
ake f
or
her.
I m
ad
e s
om
e d
evi
ces
for
Mic
hael
[Van
ner]
. T
here
is
a g
rou
p a
t M
IT t
hat
use
s so
me o
f th
e d
evi
ces
that
Im
ad
e h
ere
. W
e h
ave
th
e r
eso
nato
rs t
hat
we u
se f
or
the c
ooli
ng
exp
eri
men
t.M
akin
g n
ew
reall
y sh
ort
cavi
ty r
eso
nato
rs f
or
som
e o
ther
exp
eri
men
ts.
Th
ere
is
alw
ays
som
eth
ing
. A
nd
an
ytim
e s
tuff
need
s to
be d
on
e,
like r
eall
y h
igh
pre
ciso
n,
like m
icro
scop
y. L
ike t
he b
eat
exe
peri
men
t, t
hey
wan
t to
see t
he s
ize o
f th
eir
beat
[???
]. A
nyt
hin
g t
hat
goes
on
ou
tsid
e o
f th
e l
ab
th
at
we c
urr
en
tly
have
. S
o a
nyt
hin
gth
at
need
s to
be d
on
e i
n l
ike a
cle
an
room
.
32
.
Rein
hard
So y
ou
do t
his
alo
ne?
Or
is t
here
som
eb
od
y els
e?
33
.G
arr
ett
Sim
on
[G
röb
lach
er]
for
a w
hil
e w
as
goin
g t
o C
orn
ell
[U
niv
ers
ity]
. S
imon
Grö
bla
cher?
I n
eve
r sa
y h
is l
ast
nam
e p
rop
erl
y eve
r. H
e w
ou
ld g
o t
o C
orn
ell
an
dd
o t
he f
ab
rica
tion
. H
e i
s als
o c
ap
ab
le o
f d
oin
g t
he f
ab
rica
tion
; in
a m
ore
lim
ited
sen
se.
He c
an
make t
hose
mech
an
ical
reso
nato
rs,
bu
t n
ot
as
like..
. I
mean
I h
ave
don
e m
acr
ofa
b s
ince
19
99
or
20
00
. S
o i
t's
just
mu
ch m
ore
lik
e v
ari
ety
, w
hic
h I
'mst
ill
very
good
at.
Bu
t I
thin
k h
e i
s als
o b
ett
er.
I m
ean
his
focu
s is
at
the c
ooli
ng
exp
eri
men
t. S
o i
t's
bett
er
for
him
to n
ot
have
to g
ot
to t
he f
ab
, th
at'
s n
ice.
So i
t's
pre
dom
inan
tly
then
me.
Bu
t I
wou
ld s
ay:
me 9
0%
, S
imon
10
%.
34
.
Rein
hard
Ok.
So a
lth
ou
gh
not
work
ing
here
, h
e i
s g
ivin
g s
om
e i
np
ut.
35
.
Zu
ku
nft
sau
ssic
ht
Rein
hard
Do h
ave
an
y p
lan
s or
pro
spect
s w
hat
you
are
goin
g t
o d
o f
utu
rew
ise?
36
.G
arr
ett
I d
on
't k
now
, I
don
't k
now
. T
hat'
s act
uall
y b
een
a p
ain
, it
has
been
th
ou
gh
. C
au
se I
have
n't
reall
y p
ut
a l
ot
of
eff
ort
in
to i
t. A
nd
I d
on
't r
eall
y kn
ow
, w
hat
I w
an
na d
o.
Iw
ork
ed
for
the i
nd
ust
ry,
then
I w
as
at
Liv
erm
ore
, th
en
here
an
d t
hen
...
I w
as
goin
g
37
.
C Transcription of Interviews
106
back
an
d f
ort
h t
hin
kin
g a
bou
t aca
dem
ic p
osi
tion
s. B
ut
it d
oesn
't..
. R
igh
t n
ow
it'
sso
rt o
f le
an
ing
aw
ay
from
th
at.
I d
on
't k
now
wh
at
I w
an
na d
o.
Rein
hard
So i
t's
just
...
Leave
it
op
en
an
d s
ee w
hat
is g
oin
g t
o c
om
e.
An
d w
ait
for
that.
38
.
Fasz
inati
on
an
der
Qu
an
ten
mech
an
ik
Rein
hard
I m
ean
we a
lread
y ta
lked
ab
ou
t it
, b
ut
cou
ld y
ou
tell
wh
at
fasc
inate
s yo
u a
bou
t li
ke
qu
an
tum
mech
an
ics?
Or
more
[exp
lici
t],
the s
tuff
th
at
is d
on
e h
ere
, b
asi
call
y in
th
eexp
eri
men
ts?
39
.
Garr
ett
I ju
st l
ike t
he c
on
cep
t of
like..
. Ju
st e
xpla
inin
g t
he c
on
cep
t of
the w
ork
to
som
eb
od
y is
cra
zy t
o t
hin
k a
bou
t. C
au
se t
he s
ize s
cale
s are
very
diff
ere
nt.
Isn
'tth
at
triv
al?
Say,
if
you
make a
sin
gle
ph
oto
n s
up
erp
osi
tion
, or
do s
om
eth
ing
lik
eop
tica
l en
tan
gle
men
t exp
eri
men
t. B
ut
to t
ake i
t to
a f
air
ly m
acr
osc
op
ic m
ech
an
ical
syst
em
. I
mean
I g
o t
o t
he c
lean
room
, I
start
do s
om
e t
hin
gs
wit
h m
y h
an
ds
an
d i
nth
e e
nd
you
have
a l
ittl
e r
eso
nato
r; r
igh
t. A
nd
peop
le s
ay
you
can
see w
ith
you
reye
, alm
ost
. It
's a
mazi
ng
to t
hin
k t
hat
you
cou
ld t
hen
do,
say
in t
he l
on
g r
un
, h
ave
som
e -
- n
ow
we c
ou
ldn
't d
o -
- b
ut
som
e m
ass
ive s
up
erp
ost
ion
, w
here
you
have
th
isth
ing
both
sta
tic
an
d d
isp
laci
ng
. S
o s
om
e z
ero
-poin
t m
oti
on
of
the t
hin
g a
nd
th
en
som
e v
ibra
tion
am
pli
tud
e o
f th
e t
hin
g s
imu
ltan
iou
sly.
I t
hin
k t
his
is
reall
y co
ol.
Aco
ol
con
cep
t. I
t is
ju
st i
ntr
igu
ing
to t
he p
oin
t th
at
peop
le a
re l
ookin
g a
t th
is.
An
dth
ere
is
all
kin
ds
of
fun
ky.
.. I
use
d t
o d
o t
his
stu
die
s of
these
non
-lin
ear
reso
nan
ces,
class
ical
non
-lin
ear
reso
nan
ces.
Th
ey
can
be r
eall
y fu
nn
y st
uff
. S
o t
hese
th
ing
sh
ave
th
is h
yste
resi
s. B
ut
if y
ou
had
a q
uan
tum
reso
nato
r th
at
was
cap
ab
le o
f d
oin
gth
at,
it
wou
ld ju
st l
ead
to,
I d
on
't k
now
if
you
eve
n c
all
th
is t
un
neli
ng
. B
ut
it c
ou
ldh
op
betw
een
th
ose
tw
o s
tate
s...
40
.
Rein
hard
...w
ith
noth
ing
in
betw
een
...
41
.G
arr
ett
Yeah
. S
o i
t's
fasc
inati
ng
to t
hin
k a
bou
t th
ing
s li
ke t
hat.
I t
hin
k i
t's
more
of
the s
ize
scale
. B
eca
use
a l
ot
of
these
con
cep
ts h
ave
been
don
e.
You
kn
ow
.4
2.
Rein
hard
So a
re t
hey
sett
led
for
you
? O
r are
th
ey
stil
l kin
d o
f in
trig
uin
g?
43
.G
arr
ett
So I
wou
ld s
ay,
in
my
min
d e
very
thin
g ju
st s
eem
s to
be a
tech
nic
al
hu
rdle
. L
ike i
t is
ph
ysic
all
y p
oss
ible
. N
ot
to i
nfi
nit
y, b
ut
to a
very
larg
e s
cale
. I
don
't s
ee a
ny
road
blo
cks
there
. It
's ju
st a
tech
nic
al
chall
en
ge i
sola
tin
g t
his
th
ing
pro
perl
y. T
hat'
sth
e w
ay
I se
e i
t.
44
.
Rein
hard
So t
he c
on
cep
t is
th
ere
. T
he t
heory
says
it
work
s, s
o..
.?4
5.
Garr
ett
Th
at'
s tr
ue.
I m
ean
th
eory
[??
?] w
ork
s fo
r, r
igh
t n
ow
, u
p t
o s
om
eth
ing
lik
e t
hese
sort
of
reso
nato
rs,
we a
re l
ookin
g a
t. S
om
eth
ing
th
at'
s on
ly i
n t
he o
rder
of
som
eh
un
dre
ds
of
nan
og
ram
s. T
hat'
s fe
asa
ble
. If
you
wan
na g
o m
uch
larg
er
than
th
at,
no.
At
the s
am
e t
ime y
ou
see r
esu
lts
like f
rom
LIG
O [
Lase
r In
terf
ero
mete
rG
ravi
tati
on
al
Wave
Ob
serv
ato
ry],
th
e g
ravi
tati
on
al
wave
typ
e t
hin
g.
An
d t
hey
have
mu
lti
kil
og
ram
mir
rors
an
d t
hey
are
gett
ing
dow
n t
o f
ew
hu
nd
red
ph
on
on
s[q
uasi
part
icle
, w
hic
h r
ep
rese
nts
an
exc
ited
sta
te o
f th
e m
od
es
of
vib
rati
on
s of
ela
stic
str
uct
ure
s of
inte
ract
ing
part
icle
s. T
he s
mall
er
the n
um
ber
of
ph
on
on
s, t
he
close
r yo
u a
re a
t th
e g
rou
nd
sta
te o
f th
e s
yste
m a
nd
to a
qu
an
tum
reg
ime.]
. S
o
46
.
hon
est
ly s
eein
g t
hat,
it
makes
me t
hin
k i
t w
ou
ldn
't b
e t
hat
mu
ch h
ard
er
to k
eep
pu
shin
g t
hat.
Th
at'
s h
um
on
gou
s.R
ein
hard
So t
his
is
als
o a
n i
nte
rest
ing
way
just
to g
o t
here
, p
ush
tech
nic
all
y th
e l
imit
s an
dse
e w
hat
the o
utc
om
e i
s? B
e s
urp
rise
d,
or
not.
47
.
Helf
en
Exp
eri
men
te d
em
Vers
tän
dn
is?
Rein
hard
Do y
ou
see t
hese
exp
eri
men
ts a
s so
meth
ing
th
at
mig
ht
help
in
un
ders
tan
din
g,
like
the i
ntr
igu
ing
part
s?4
8.
Garr
ett
I th
ink s
o. T
he t
hin
g t
hat
alw
ays
com
es
up
an
d f
or
me i
t's
more
lik
e -
- w
hat'
s th
eri
gh
t w
ord
--
para
din
g o
r [?
??].
.. B
eca
use
th
eore
tica
l m
y b
ack
gro
un
d i
s n
ot
nearl
yth
at
stro
ng
.
49
.
(no s
peaker)
[lit
tle i
nte
rru
pti
on
]5
0.
Garr
ett
Ok.
Wh
at
was
the l
ast
qu
est
ion
? W
e h
ave
to r
ew
ind
an
d s
ee.
51
.R
ein
hard
Oh
, if
lik
e d
oin
g t
he e
xperi
men
ts c
ou
ld h
elp
in
un
ders
tan
din
g t
he i
ntr
igu
ing
thin
gs.
Or
just
gett
ing
sett
led
ab
ou
t it
.5
2.
Garr
ett
I co
me f
rom
a t
ota
lly
diff
ere
nt
back
gro
un
d,
such
as
weir
d t
hat
the w
ay
I th
ink
ab
ou
t it
mig
ht
be d
iffere
ntl
y. W
hic
h i
s in
tere
stin
g,
I u
nd
ers
tan
d.
Wh
en
peop
leta
lkin
g a
bou
t all
th
is q
uan
tum
cla
ssic
al
tran
siti
on
: Is
th
ere
lik
e a
bou
nd
ary
in
betw
een
th
ese
th
ing
s? M
ine i
s: I
don
't s
ee t
hat
they
are
an
y d
iffere
nt.
Bu
t on
e i
sju
st s
om
e e
xtre
me f
orm
of
the o
ther.
So I
th
ink i
t w
ou
ld b
e n
ice t
o s
how
th
at
you
can
take s
om
eth
ing
mass
ive a
nd
see q
uan
tum
eff
ect
s in
it.
I d
on
't r
eall
y kn
ow
how
man
y p
eop
le i
n t
his
field
or
in t
his
are
a,
wou
ld e
very
th
ink t
here
is
som
e s
ud
den
chan
ge w
hen
you
go f
rom
on
e s
ide o
f p
hys
ics
to t
he o
ther.
I t
hin
k a
nyb
od
y d
oin
gth
is,
it'd
be s
urp
risi
ng
if
they
thou
gh
t th
at
way.
I'd
act
uall
y b
e s
urp
rise
d,
if t
here
is
an
y [?
??]
that
act
uall
y als
o t
hin
ks
that
way.
Bu
t it
'd b
e n
ice t
o p
roof,
th
at
you
can
take s
om
eth
ing
th
at
mass
ive a
nd
sh
ow
som
e q
uan
tum
eff
ect
s in
it.
53
.
I th
ink t
he m
ost
in
tere
stin
g,
like t
ech
nic
al,
th
ing
to s
tud
y, i
s to
see w
hat
cau
ses
itto
ap
pear,
to b
e c
om
ple
tely
...
Wh
at
cau
ses
it t
o b
e c
lass
ical,
I g
uess
. S
o i
n t
hat
sen
se,
in t
hat
dir
ect
ion
you
need
to s
tud
y th
e d
eco
here
nce
mech
an
ism
s th
at
work
.T
hat
wou
ld k
ill
those
qu
an
tum
eff
ect
s in
th
ese
big
sys
tem
s. S
o t
here
's l
ots
of
neat
pro
posa
ls,
like t
his
Pen
rose
mod
el
an
d t
hese
oth
er
on
es
I d
on
't k
now
th
e d
eta
ils
of
an
d t
he n
am
es
of.
It'
d b
e a
[??
?] t
o s
ee l
ike s
ay:
We c
an
pre
pare
, fi
st s
om
e n
an
om
ech
an
ical
reso
nato
rs a
nd
larg
er
mic
rom
ech
an
ical
reso
nato
rs,
an
d e
ven
tuall
yth
ose
LIG
O s
cale
, li
ke k
ilog
ram
str
uct
ure
. A
nd
th
en
pre
pare
it
in s
om
e s
tate
an
dth
en
let
it s
it a
nd
evo
lve,
an
d ju
st d
ie b
ack
to s
om
e b
ori
ng
, d
um
b [
class
ical
state
].H
ow
fast
is
that
tim
e s
cale
hap
pen
ing
on
. W
hat
does
the t
heory
sh
ow
it
hap
pen
son
. A
nd
th
en
com
pare
th
is a
nd
see w
hat'
s it
lik
e.
54
.
It s
ort
of
goes
back
to w
hat
I sa
id e
arl
ier,
bu
t in
th
e e
nd
eve
ryth
ing
is
just
...
If y
ou
take a
nyt
hin
g a
nd
pro
perl
y is
ola
te a
t le
ast
on
e d
eg
ree o
f fr
eed
om
or
on
e t
hin
g t
hat
you
can
get
som
e c
hara
cteri
stic
of.
Have
th
e m
easu
rem
en
t h
as
to b
e s
om
e p
oin
tw
ere
you
can
see q
uan
tiza
tion
, yo
u c
an
see s
om
e q
uan
tum
eff
ect
s in
th
at
state
. If
you
pro
perl
y re
move
d i
t's
con
nect
ion
s fr
om
eve
ryth
ing
. W
hic
h b
eco
mes
just
more
tech
nic
all
y ch
all
en
gin
g a
s yo
u y
ou
move
up
in
sca
le.
So i
t's
just
kin
d o
f n
eat
toth
ink a
bou
t th
at.
Th
at'
s m
ayb
e n
ot
the m
ost
exc
itin
g o
utc
om
e,
to m
e i
t w
ou
ld b
en
eat
to s
ee.
55
.
107
Rein
hard
So t
he e
xperi
men
ts,
at
least
try
...
56
.G
arr
ett
Sh
ort
term
all
th
ese
exp
eri
men
ts fi
rst
have
to g
et
there
; to
ward
s re
peata
ble
... S
o i
fyo
u g
o b
ack
an
d l
ook a
t li
ke t
he i
on
tra
pp
ing
or
ato
m c
ooli
ng
. A
nd
peop
le w
ork
ed
for
a l
on
g t
ime a
nd
now
it'
s, I
wou
ldn
't c
all
it
rou
tin
e,
bu
t it
's f
air
ly r
ou
tin
e t
op
rep
are
th
ese
sta
tes.
An
d n
ow
you
can
do l
ike v
ery
beau
tifu
l p
hys
ics
wit
h t
hese
syst
em
s. S
o w
e a
re a
t th
e p
oin
t w
ere
we'r
e d
eve
lop
ing
th
e b
ack
gro
un
d s
tep
s to
get
there
. It
's r
eall
y ch
all
en
gin
g,
bu
t th
ere
wil
l b
e a
poin
t li
ke y
ears
fro
m n
ow
, w
hen
peop
le l
ook b
ack
an
d s
ay:
Now
it'
s d
on
e,
now
we c
an
bu
y a m
od
el
an
d p
ress
ab
utt
on
. A
nd
you
do i
t, r
igh
t. S
o w
e a
re a
t th
e m
ore
diffi
cult
sta
ge o
f ju
st p
rep
ari
ng
,ju
st l
ayi
ng
th
e g
rou
nd
wort
h t
o g
et
to t
he q
uan
tum
reg
ime w
ith
th
e d
evi
ces;
rig
ht.
On
ce t
hey
are
th
ere
, th
en
you
can
sta
rt l
ookin
g a
t w
hat
sort
of
ph
ysic
s ca
n y
ou
do
wit
h t
hese
sys
tem
s. P
rep
are
som
e e
nta
ng
led
sta
te o
r su
perp
osi
tion
sta
te o
f th
em
ech
an
ics.
Let
them
evo
lve i
n t
ime a
nd
do t
hese
measu
rem
en
ts.
57
.
I m
ean
it'
s alr
ead
y h
ere
. B
eca
use
th
e C
lela
nd
gro
up
at
San
ta B
arb
ara
[htt
p:/
/ww
w.p
hys
ics.
ucs
b.e
du
/~cl
ela
nd
gro
up
/] h
ad
th
is d
em
on
stra
tion
last
year.
Th
is t
hin
g w
as
rap
idly
deca
yin
g,
bu
t n
eat
ele
ctro
mech
an
ical
reso
nato
r. J
ust
beca
use
it'
s so
hig
h f
req
uen
cy t
hey
can
cool
it t
o t
he g
rou
nd
sta
te.
It w
as
cou
ple
dto
th
is t
wo l
eve
l q
ub
it.
Th
ey
cou
ld w
rite
sin
gle
ph
on
on
s on
to i
t. R
ead
it
ou
t. T
hey
cou
ld p
ut
sin
gle
ph
on
on
su
perp
osi
tion
sta
tes
in i
t. T
his
th
ing
was
a l
arg
e s
tru
ctu
re.
Th
is i
s als
o a
mic
ron
-sca
le d
evi
ce.
58
.
Rein
hard
Nic
e!
59
.G
arr
ett
We a
re b
asi
call
y th
ere
. W
e a
re o
n t
he b
rin
k w
here
it'
s li
ke b
ein
g a
ble
to r
eali
zeth
is.
An
d t
hen
wh
at
you
do n
ext
? S
o t
hen
you
pre
pare
, ju
st f
or
sort
of
glo
ry,
these
fan
zy q
uan
tum
sta
tes,
eve
n t
hou
gh
th
ey
may
not
last
for
an
y so
rt o
f ti
me. B
ut
it's
just
to s
how
th
at
we c
an
do t
his
. A
nd
th
en
wh
en
it
beco
mes
more
rep
rod
uca
ble
to
create
th
ese
th
ing
s, s
tud
y h
ow
th
ey
surv
ive.
An
d t
hen
you
can
do a
ll t
he s
am
e s
ort
of
exp
eri
men
ts y
ou
did
wit
hin
op
tica
l d
om
ain
[b
ut]
wit
h t
hese
larg
e m
ech
an
ical
syst
em
s. D
o t
hey
beh
ave
th
e s
am
e?
60
.
It's
neat
to s
ee,
com
ing
ou
t of
like..
. W
e s
tart
ed
at
IQO
QI
[In
stit
ut
fuer
Qu
an
ten
op
tik u
nd
Qu
an
ten
info
rmati
on
, A
kad
em
ie d
er
Wis
sen
sch
aft
en
], s
o i
nA
nto
n Z
eil
ing
ers
in
stit
ute
th
ere
. S
o h
e s
tart
ed
way
back
wit
h t
he n
eu
tron
exp
eri
men
ts,
op
tica
l exp
eri
men
ts.
An
d t
hen
th
e e
xten
sion
to l
arg
er
stu
ff,
like
Mark
us
Are
nd
ts w
ork
. A
nd
so t
hen
you
keep
walk
ing
up
th
e s
ize s
cale
. N
ow
we
have
fu
ll m
icro
fab
rica
ted
devi
ces.
It'
s n
eat
to s
ee t
he p
rog
ress
ion
. It
's r
eall
y co
ol
that
they
[Mark
us
Are
nd
t g
rou
p]
are
doin
g t
his
basi
c, a
rch
ety
pal
dou
ble
sli
texp
eri
men
t. F
irst
wit
h t
he C
60
[fu
llere
ne]
an
d n
ow
it'
s li
ke p
rote
ins
an
d c
razy
stu
ff.
61
.
Rein
hard
On
pap
er,
in
pri
nci
ple
, it
is
qu
ite n
ice a
nd
easy
, an
d n
ot
com
pli
cate
d a
t all
. Yo
u ju
st[h
ave
to i
mp
lem
en
t it
][sa
rcsm
]6
2.
Garr
ett
Th
e b
asi
c p
hys
ics
ob
viou
sly
have
in
terf
ere
nce
occ
ur.
It'
s th
e s
am
e.
Be i
t si
ng
lep
hoto
n,
be i
t b
uck
y b
all
[C
60
, fu
llere
ne];
you
kn
ow
. Ju
st t
he b
uck
y b
all
has
lots
more
deg
rees
of
freed
om
. S
o t
hey
can
see s
om
e n
eat
thin
gs.
Eve
n t
hou
gh
th
ese
are
lau
nch
ed
ou
t of
an
ove
n,
wit
h s
om
eth
ing
lik
e i
nte
rnal
tem
pera
ture
s of
hu
nd
red
s of
Celc
ius
at
least
. A
nd
th
at
these
th
ing
s d
on
't ju
st i
nst
an
ten
iou
sly
deco
here
. T
hey
just
eve
n c
an
sti
ll s
ee e
ffect
s. T
hat
is v
ery
im
pre
ssiv
e.
Bu
t th
esa
me a
rgu
men
ts c
an
be m
ad
e o
f li
ke..
. T
his
is
som
eth
ing
som
e p
ers
on
s p
ut
in t
he
lab
, m
ad
e w
ith
th
eir
han
ds,
bro
ug
ht
ou
t, w
eld
ed
in
to a
mach
ine.
You
kn
ow
, if
you
63
.
make t
he c
on
dit
ion
s ri
gh
t yo
u c
an
cool
to t
he g
rou
nd
sta
te a
nd
th
en
see t
hese
eff
ect
s. I
th
ink i
t's
exc
itin
g.
I d
on
't k
now
if
it m
akes
it m
ore
tan
gib
le t
o t
he g
en
era
l p
ub
lic,
bu
t it
's..
. O
k,
wh
en
you
have
a s
ing
le e
lect
ron
, or
giv
e a
neu
tron
or
those
th
ing
s. P
eop
le w
ou
ld k
now
the w
ord
s, b
ut
they
have
no i
dea w
hat
that
thin
g i
s. R
igh
t? A
t n
ext
we a
re m
ovi
ng
up
to s
ay
a m
ole
cule
, li
ke a
bu
cky
ball
[C
60
, fu
llere
ne].
Th
at
is s
tart
ing
to g
et
ali
ttle
more
...
You
can
sh
ow
pic
ture
s of
a s
occ
er
ball
, th
at'
s w
hat
it l
ooks
like.
It's
beco
min
g m
ore
tan
gib
le t
o t
he n
orm
al
pers
on
. A
nd
th
en
as
you
pro
gre
ss u
p i
n t
he
size
of
clu
sters
an
d d
iffere
nt
org
an
ic m
ole
cule
s. T
hen
it
beco
mes
more
rele
van
t.A
nd
th
e s
am
e t
hin
g,
I th
ink f
or
us.
Now
we a
re s
tart
ing
to m
ake s
om
e m
ech
an
ical
reso
nato
rs,
the e
xtre
me a
gain
is
this
LIG
O m
irro
r, t
hat
is m
ass
ive,
like ju
st a
gia
nt
fat
din
er
pla
te.
Som
eth
ing
you
cou
ld a
ctu
all
y g
o s
ee t
hat.
You
cou
ld t
ell
th
em
wh
at
it w
as
doin
g.
Th
en
it
beco
mes
mu
ch,
mu
ch m
ore
tan
gib
le t
o t
he g
en
era
l p
ub
lic.
64
.
Rein
hard
At
least
in
creasi
ng
som
e k
ind
of
rele
van
ce.
65
.G
arr
ett
Yeah
. E
ven
if
it's
ju
st s
ize g
ain
. O
r so
meth
ing
som
eon
e c
an
see.
Or
som
eth
ing
th
at
you
are
fam
ilia
r w
ith
. Yo
u c
an
alw
ays
tu
rn t
o d
esc
rib
e o
ur
devi
ces
like i
t's
a m
irro
r,a t
un
ig f
ork
. It
's s
om
eth
ing
more
th
at
they
can
im
ag
ine a
s a l
ittl
e r
eso
nato
r. R
igh
t?Vers
us
like I
have
a n
eu
tron
. [l
au
gh
s] T
o s
om
e d
eg
ree t
he p
hys
ics
are
n't
very
diff
ere
nt,
bu
t ju
st a
noth
er
pla
tform
to d
isp
lay.
An
d t
here
are
ob
viou
sly
new
th
ing
sth
at
com
e i
nto
pla
y.
66
.
Inte
rpre
tati
on
en
Rein
hard
Are
you
som
eh
ow
in
to t
he d
iscu
ssio
n a
bou
t in
terp
reta
tion
of
qu
an
tum
mech
an
ics?
67
.G
arr
ett
Th
e p
rob
lem
is.
.. T
hat'
s g
ett
ing
to f
ar
ou
t fo
r m
e s
om
eti
mes.
I m
ean
ju
st b
eca
use
...
Th
at'
s on
e t
hin
g I
'm a
ctu
all
y sl
igh
tly
dis
ap
poin
ted
wit
h m
yself
here
so f
ar.
I t
hin
kyo
u ju
st g
et
cau
gh
t u
p i
n t
he w
ork
th
at
you
have
to d
o.
Wh
en
I fi
rst
got
here
Ip
rom
ised
mys
elf
: O
k,
I re
all
y si
t d
ow
n a
nd
stu
dy
like b
asi
c q
uan
tum
mech
an
ics
tom
ore
th
oro
ug
hly
part
icip
ate
in
th
e c
on
vers
ati
on
s. B
ut
at
som
e p
oin
t yo
u h
ave
to
stop
, ca
use
you
have
you
r d
ay-
to-d
ay
stu
ff t
hat
you
need
to d
o.
Un
fort
un
ate
ly n
o.
I'm
act
uall
y re
all
y b
ad
wit
h t
hat.
68
.
Rein
hard
Bu
t yo
u s
ee t
hat
there
is
som
e k
ind
of
dis
cuss
ion
goin
g o
n?
69
.G
arr
ett
I se
e t
hose
dis
cuss
ion
s. I
feel
like h
ere
...
Hon
est
ly t
hat
is p
ure
ly m
y in
terp
reta
tion
,b
ut
it s
eem
s li
ke b
eca
use
to s
om
e d
eg
ree e
very
bod
y b
ran
ches
ou
t fr
om
An
ton
[Zeil
ing
er]
. T
here
is
not
a h
ug
e d
ivers
ity
in s
ort
of
min
d s
et.
Lik
e e
very
on
e s
ort
of
ag
gre
es.
Man
y ti
ny
deta
ils
that
peop
le d
isag
gre
e w
ith
, b
ut
it's
...
Th
ere
is
on
e t
eam
here
. T
here
is
like o
ne s
ing
le i
nte
rpre
tati
on
th
at
wil
l b
e f
oll
ow
ed
here
. B
ut
that'
sju
st w
hat
I w
ou
ld g
uess
.
70
.
Rein
hard
Pla
usi
ble
.7
1.
Garr
ett
Yeah
. I
see e
xam
ple
s w
hen
vis
itors
wil
l co
me a
nd
th
ere
wil
l b
e d
iscu
ssio
ns
wit
h t
he
visi
tors
. T
hey
then
dis
ag
ree w
ith
wh
at
mayb
e s
ort
of
a n
orm
here
. B
ut
it s
eem
s li
ke
the d
iscu
ssio
n w
ith
in t
he g
reate
r, l
ike u
niv
ers
ity,
IQ
OQ
I, a
nd
th
e g
rou
ps
that
inte
ract
wit
h I
QO
QI
from
th
e u
niv
ers
ity.
Eve
ryb
od
y se
em
s to
be o
n t
he s
am
e t
rain
of
thou
gh
t. T
his
is
ou
r in
terp
reta
tion
an
d t
hat
is h
ow
th
ing
s are
.
72
.
C Transcription of Interviews
108
Rein
hard
I se
e.
So y
ou
are
als
o i
n t
his
set
of
inte
rpre
tati
on
.7
3.
Garr
ett
Kin
d o
f. I
th
ink I
have
n't
been
exp
ose
d t
o a
nyt
hin
g e
lse.
74
.R
ein
hard
Th
e q
uest
ion
is
wh
eth
er
it i
s of
an
y re
leva
nce
? P
rop
ab
ly n
ot
for
the d
ay-
to-d
ay
work
, b
eca
use
...?
75
.
Garr
ett
I d
on
't k
now
if
this
is
tru
e,
bu
t...
Ob
viou
sly
the p
eop
le w
ho c
om
e h
ere
, to
som
ed
eg
ree a
gre
e w
ith
wh
at'
s g
oin
g o
n.
So f
oll
ow
th
at
inte
rpre
tati
on
. A
nd
th
en
als
o i
tw
ou
ld b
e h
ard
er
if y
ou
cam
e w
ith
a c
om
ple
tly
con
trad
icto
ry v
iew
to s
ell
you
rself
to
com
e i
nto
th
e d
ep
art
men
t li
ke t
hat.
As
I sa
id f
or
me,
I h
ave
on
ly b
een
exp
ose
d t
oth
is h
on
est
ly.
76
.
tech
nis
ch
er
Fort
sch
ritt
Rein
hard
How
do y
ou
see,
that
is k
ind
of
an
ob
viou
s q
uest
ion
,...
How
do y
ou
see t
he
infl
uen
ce o
f th
e t
ech
nic
al
en
han
cem
en
ts t
hat
were
goin
g o
n.
Pro
pab
ly t
hose
exp
eri
men
t w
ou
ldn
't b
e p
oss
ible
if
on
e c
ou
ld n
ot
en
gin
eer
those
th
ing
s.
77
.
Garr
ett
Th
is i
s on
all
fro
nts
th
ou
gh
. I
mean
th
e t
hin
g i
s yo
u h
ave
to,
at
least
for
ou
rexp
eri
men
ts s
peci
fica
lly,
have
very
hig
h p
erf
orm
an
ce,
like l
ow
dam
pin
g,
hig
hre
flect
ivit
y, v
ery
pre
cise
geom
etr
y m
ech
an
ical
reso
nato
rs,
rig
ht.
Th
at
reli
es
full
yon
mic
ro-n
an
o f
ab
rica
tion
tech
nolo
gie
s, l
ike h
ave
th
eir
root
in i
nte
gra
ted
cir
cuit
s.S
o l
ike f
rom
th
e fi
ftie
s. A
nd
eve
ry t
ime t
hat
ad
van
ces,
th
en
we c
an
bu
ild
off
th
ose
ad
van
cem
en
ts,
rig
ht.
Bu
t eve
ryth
ing
in
th
e l
ab
...
I th
ink i
t's
tru
e o
f all
sci
en
ce t
oso
me d
eg
ree t
hat
like t
hese
eff
ect
s h
ave
been
th
ere
.
78
.
It t
akes
som
eon
e t
o c
om
e u
p w
ith
a t
heory
to l
ook f
or
it i
n t
he fi
rst
pla
ce o
r yo
uacc
iden
tall
y d
isco
ver
it,
wh
ich
is
als
o p
oss
ible
. B
ut
then
to e
xperi
men
tall
y m
easu
rean
y of
these
th
ing
s th
ere
has
to b
e a
dva
nce
men
ts i
n t
he t
ools
to d
o t
he
measu
rem
en
t. A
ll t
he b
asi
c ele
ctro
nic
s, ju
st s
tuff
lik
e t
he o
scil
losc
op
e,
spect
rum
an
aly
zers
, w
hate
ver
it m
ay
be.
As
they
beco
me m
ore
sen
siti
ve,
then
it'
s easi
er
toso
rt o
f fi
nd
ou
t th
ese
tin
y fu
nn
y th
ing
s. M
ost
of
the o
bvi
ou
s eff
ect
s are
kin
d o
fg
on
e.
Un
less
you
com
e u
p w
ith
an
en
tire
ly n
ew
ph
ysic
al
fact
th
at
was
som
eh
ow
ove
rlooked
or
un
der
som
e c
on
dit
ion
s so
meth
ing
pop
s u
p.
Th
at'
s ra
re.
So y
ou
are
reall
y lo
okin
g f
or
hig
her
ord
er
thin
gs
that
peop
le d
id n
ot
an
tici
pate
, d
idn
't e
xpect
or
cou
ldn
't m
easu
re ju
st b
efo
re;
rig
ht.
79
.
I m
ean
for
us
it's
...
You
kn
ow
we a
re d
eali
ng
wit
h r
ad
iati
on
pre
ssu
re.
So w
e s
ort
of.
.. a
mp
lifi
y is
not
the c
orr
ect
tech
nic
al
term
, b
ut
we m
ake t
his
vis
ible
. B
eca
use
we h
ave
th
is c
avi
ty a
nd
beca
use
we a
re m
od
ifyi
ng
th
e d
ynam
ic,
the r
esp
on
se o
fth
e m
ech
an
ical
reso
nato
r. W
e a
lso h
ave
an
exp
eri
men
t ou
t, w
hic
h i
s kin
d o
f fu
n,
wh
ere
we ju
st h
ave
th
ese
larg
e c
an
tile
vers
. L
arg
e?!
I c
all
th
em
larg
e,
beca
use
th
ey
are
th
ree m
illi
mete
rs.
Bu
t th
ey
are
3 m
illi
mete
rs b
y 6
mic
ron
s b
y 5
mic
ron
s. S
oth
ey
are
lik
e l
ittl
e h
air
s. W
e u
se r
ad
iati
on
pre
ssu
re ju
st t
o d
efl
ect
th
ose
, I
mean
just
to d
rive
th
em
in
to r
eso
nan
ce.
80
.
An
d t
he n
ice t
hin
g i
s, w
e c
an
fu
lly
do t
his
on
a t
ab
le t
op
. T
hat'
s b
eca
use
I h
ad
ave
ry n
ice l
ase
r so
urc
e.
It t
ook a
dva
nce
men
ts t
o m
ake t
his
lik
e n
ice l
ittl
e l
ase
r. I
t's
a g
reen
narr
ow
lin
e d
iod
e l
ase
r, I
can
mic
rofa
bri
cate
th
is t
hin
g [
the c
an
tile
ver]
.B
eca
use
th
e m
ate
rials
ava
ilab
le n
ow
ad
ays
are
in
all
very
nic
e;
sort
of
hig
h q
uali
tym
ate
rial.
Th
e m
icro
fab
rica
tion
has
gott
en
to t
he p
oin
t w
here
I c
an
make t
his
com
ple
x st
ruct
ure
. A
nd
th
en
I h
ave
som
e r
ead
ou
t sy
stem
wit
h t
his
sp
lit
ph
oto
dio
de,
wh
ere
I c
an
measu
re t
he d
isp
lace
men
t of
this
lit
tle b
eam
. O
n t
he t
ab
le I
can
81
.
now
bu
ild
th
is s
et
up
th
at
I ca
n s
how
you
th
e m
om
en
tum
tra
nsf
er
wit
h p
hoto
ns
refl
ect
ing
of
the s
urf
ace
, m
akin
g a
mech
an
ical
syst
em
move
. W
hic
h i
s alr
ead
y...
Th
ere
is
not
like f
un
dam
en
tal
qu
an
tum
eff
ect
s th
ere
un
less
you
sta
rt g
et
sin
gle
ph
oto
ns.
I m
ean
th
is i
s p
hys
ics,
th
at
in p
rin
cip
le s
hou
ld h
ave
alw
ays
been
th
ere
, b
ut
it's
ju
stso
hard
to s
ee.
So t
he o
rig
inal
exp
eri
men
ts i
n t
hat
are
a w
ere
in
19
01
, w
here
th
isg
uy
Leb
ed
ev,
th
en
Nic
hols
/Hu
ll [
Ern
est
Fox
Nic
hols
an
d G
ord
on
Ferr
ie H
ull
], t
hese
am
eri
can
gu
ys.
Th
ey
had
...
If y
ou
look a
t p
ictu
res
of
their
exp
eri
men
ts,
they
basi
call
y h
ave
som
e m
ass
ive l
igh
t so
urc
e,
these
len
ses,
th
ese
sil
vere
d m
irro
rs n
eed
hu
ge [
???]
arc
hs.
Th
ese
th
ing
s ta
ke u
p a
wh
ole
room
. A
nd
th
ey
are
measu
rin
gte
en
y, t
een
y, t
iny
forc
es
an
d t
iny
dis
pla
cem
en
ts.
An
d t
hey
are
usi
ng
ju
st e
ith
er
their
eye
an
d a
sm
all
gu
ide t
o s
ee a
defl
ect
ion
. S
o i
t's
am
azi
ng
ju
st w
hat
you
can
see.
Now
we c
an
rou
tin
ely
...
Mark
us
[Asp
elm
eye
r] w
hen
he g
ave
his
An
trit
tsvo
r...
.
82
.
Rein
hard
Die
An
trit
tsvo
rlesu
ng
.8
3.
Garr
ett
I st
op
ped
cau
se I
th
ou
gh
t th
at
was
reall
y w
ron
g.
So w
e m
ad
e l
ike a
lit
tle d
em
o.
Did
you
go t
o t
hat?
84
.
Rein
hard
Yeah
, I
have
seen
th
at.
85
.G
arr
ett
So t
hat
was
this
exp
eri
men
t act
uall
y I
just
desc
rib
ed
. In
to t
he p
oin
t w
here
we
cou
ld b
uil
d i
t an
d r
oll
it
into
th
e a
ud
itori
um
an
d s
how
it.
An
d i
f yo
u'd
sh
ow
it
som
eon
e l
ike L
eb
ed
ev
or
Nic
hols
/Hu
ll,
it's
a h
un
dre
d a
nd
ten
years
late
r. S
o t
here
is a
lot
of
ad
van
cem
en
ts i
n t
ech
nolo
gy;
on
all
fro
nts
. L
ike f
rom
ju
st t
he v
ibra
tion
isola
tin
g o
pti
cal
tab
le t
o t
his
dio
de l
ase
r, t
o t
hese
ele
ctro
nic
s th
at
do t
he r
ead
ou
t.E
very
thin
g w
e d
o r
eli
es
on
ad
van
cem
en
ts i
n t
hese
tools
. T
he e
xtre
me c
ase
of
that
is m
easu
rin
g q
uan
tum
eff
ect
s. I
f w
e a
re g
oin
g t
o m
easu
re s
om
e..
. A
t so
me p
oin
tw
e h
ave
to b
e a
ble
to m
easu
re t
he r
eso
luti
on
bett
er
than
th
e z
ero
poin
t m
oti
on
of
this
mech
an
ical
reso
nato
r; r
igh
t. A
nd
ju
st t
he p
reci
sion
th
at'
s n
ece
ssary
to
measu
re t
hat
is a
bsu
rd.
It's
am
azi
ng
ly t
hat
you
can
eve
n g
et
there
. S
o g
o b
ack
ten
,tw
en
ty,
thir
ty y
ears
, it
's ju
st n
ot
poss
ible
to d
o.
Th
ese
exp
eri
men
ts c
ou
ld h
ave
been
pro
pose
d,
bu
t th
ey
wou
ld n
eve
r h
ap
pen
un
til
the t
ech
nolo
gy
cau
gh
t u
p.
86
.
Rein
hard
Do y
ou
see..
. th
is t
hin
gs
dri
vin
g t
he t
ech
nolo
gy
the o
ther
way.
Say
beca
use
th
ere
is
need
for
the e
xperi
men
ts t
o h
ave
su
ch a
pre
cisi
on
en
gin
eeri
ng
, th
at
als
o t
he
en
gin
eeri
ng
pro
fits
fro
m i
t.
87
.
Garr
ett
I th
ink o
ur
field
is
ext
rem
ely
new
, so
it'
s h
ard
to s
ee d
irect
ly t
he i
mp
act
. B
ut
ag
ain
giv
en
th
ing
s li
ke L
IGO
. T
he g
ravi
tati
on
al
wave
peop
le a
re e
ssen
tiall
y...
they
are
not
lookin
g f
or
qu
an
tum
eff
ect
s. B
ut
their
req
uir
em
en
ts a
re v
ery
sim
ilar
to o
urs
. T
hey
are
very
para
llel
to w
hat
we d
o.
I m
ean
th
ese
gu
ys h
ave
pu
shed
th
e l
imit
of
like
these
op
tica
l co
ati
ng
s to
make t
hese
hig
h r
efl
ect
ing
mir
rors
, w
hic
h y
ou
can
now
get.
.. A
ll t
he o
pti
cs w
e u
se a
re c
oate
d w
ith
stu
ff b
ase
d o
n t
ech
nolo
gy
deve
lop
ed
for.
.. d
rive
n b
y th
at
exp
eri
men
t.
88
.
Sam
e t
hin
g f
or
us
now
, w
here
we r
eall
y h
ave
...
Lik
e t
he o
ne e
xam
ple
, ca
use
th
is i
sals
o v
ery
rece
nt,
it'
s ti
ed
to s
tuff
I a
lso u
sed
to d
o.
So w
e n
eed
to a
mp
lify
very
,ve
ry,
very
low
lig
ht
leve
ls n
ow
. W
e h
ave
th
is o
pti
cal
cavi
ty,
we s
en
d i
n v
ery
, ve
ry,
very
weak l
igh
t an
d w
e w
an
na r
ead
ou
t th
e s
tate
of
lig
ht
com
ing
ou
t of
this
. A
nd
that'
s act
uall
y re
all
y to
ug
h t
o d
o.
To t
ake t
his
very
, ve
ry..
.th
is t
iny
sig
nal
ou
t of
the
nois
e a
nd
am
pli
fy i
t. A
nd
so w
e o
rdere
d..
. It
was
act
uall
y a c
om
pan
y I
use
d t
o w
ork
for.
So w
e ju
st b
ou
gh
t th
is a
mp
lifi
er
from
th
em
, w
hic
h d
id n
ot
exi
st u
p u
nti
l th
ey
start
off
eri
ng
it
a y
ear
ag
o.
An
d n
ow
it
looks
like...
We'll
see,
if i
t w
ork
ed
. B
ut
in
89
.
109
pri
nci
ple
th
at
can
en
ab
le u
s to
reall
y d
rop
th
e p
ow
er.
It
makes
a l
ot
of
thin
gs
exp
eri
men
tall
y n
icer.
For
the p
ast
year
plu
s, I
've b
een
pu
shin
g t
hem
. I
had
work
ed
on
th
ese
devi
ces
befo
re a
nd
we h
ad
a n
eed
for
som
eth
ing
lik
e t
hat.
An
d I
said
: W
e n
eed
th
is,
we
need
th
is,
we n
eed
th
is,
we n
eed
th
is.
So r
eall
y p
ush
ing
th
em
. C
au
se t
hey
were
makin
g d
evi
ces
like f
or
pro
of
of
pri
nci
ple
stu
ff.
In t
he U
S a
lot
of
is d
rive
n b
yd
efe
nce
rela
ted
stu
ff.
Th
ey
were
makin
g d
evi
ces
for
these
defe
nce
con
tract
s, b
ut
reall
y n
ot
to b
e a
pp
lied
in
an
yth
ing
. It
was
more
ju
st a
dva
nce
th
e s
tate
of
the a
rtan
d t
hen
mayb
e fi
nd
a u
se. T
hen
I h
ave
to e
or
call
th
em
, p
est
er
these
gu
ysan
d s
ay:
I k
now
you
can
meet
these
sp
ecs
, if
you
keep
try
ing
. A
nd
if
you
say
we
wil
l b
uy
them
an
d w
e w
ill
use
it.
An
d i
f w
e s
how
, w
e g
et
good
pre
ss f
or
this
an
doth
er
peop
le w
an
t to
bu
y it
. It
op
en
s a l
ittl
e m
ark
et.
It'
s sm
all
rig
ht
now
in
ou
rsp
eci
fic
field
. B
ut
there
's l
ots
of
measu
rem
en
t te
chn
olo
gy
that
can
ben
efi
t fr
om
measu
rin
g t
hese
ext
rem
ely
low
lig
ht
leve
ls,
weak l
igh
t le
vels
. S
o i
t d
oes
go b
ack
an
d f
ort
h.
I d
efi
nit
ely
th
ink i
t fe
ed
s b
ack
.
90
.
An
d s
o o
ne m
ore
th
ing
ju
st c
au
se w
e..
. T
he o
ther
on
e w
as,
an
oth
er
con
crete
exa
mp
le,
these
posi
tion
ing
sys
tem
s. T
his
very
lik
e e
sote
ric.
Very
sp
eci
fic
stu
ff w
eh
ave
to d
o t
ech
icall
y. W
e h
ave
to w
ork
at
very
low
tem
pera
ture
s an
d w
e h
ave
to
move
a l
ittl
e c
hip
[T
he c
hip
wit
h t
he c
an
tile
vers
on
it]
aro
un
d.
An
d t
here
is
ag
erm
an
com
pan
y, c
all
ed
[??
?],
that
makes
these
sys
tem
s. A
nd
th
en
th
ey.
.. O
ne
thin
g t
hat
was
alw
ays
an
noyi
ng
befo
re,
you
neve
r kn
ew
wh
ere
you
were
loca
lly.
You
cou
ld m
ove
, b
ut
I ca
n n
eve
r ask
th
e s
yste
m,
wh
ere
did
you
move
to.
Itw
ou
ldn
't k
now
. S
o i
t w
ou
ld m
ove
, m
ove
, m
ove
, m
ove
. M
ayb
e I
kn
ew
wh
ere
Ist
art
ed
, b
ut
I h
ave
no i
dea w
here
I e
nd
ed
up
for
sure
.
91
.
So t
hen
we t
alk
ed
to t
hem
an
d t
hey
said
th
at
they
were
deve
lop
ing
an
en
cod
ed
syst
em
, th
at
can
reco
rd w
here
th
e t
hin
g w
as
an
d w
e c
an
read
th
at
ou
t. W
e s
how
ed
som
e i
nte
rest
an
d w
e s
aid
yes.
An
d n
ow
th
ere
is
a l
ot
of
gro
up
s, n
ot
just
us,
bu
tth
ere
's t
on
s of
ap
pli
cati
on
s fo
r th
at
to h
ave
it.
Bu
t w
e p
ush
ed
th
em
. W
e t
hou
gh
t it
was
a fi
nis
hed
com
merc
ial
devi
ce,
bu
t it
tu
rned
ou
t it
was
more
of
a p
roto
typ
e.
Beca
use
we h
ad
an
au
tom
ate
d s
yste
m,
som
e s
oft
ware
to r
ead
ou
t w
ere
th
is t
hin
gw
as.
Bu
t th
at
did
n't
work
at
all
. I
don
't a
gre
e w
ith
it,
beca
use
we s
pen
t to
ns
of
tim
e d
eve
lop
ing
th
is s
oft
ware
, ess
en
tiall
y fo
r th
em
, to
make i
t w
ork
. A
nd
th
en
feed
back
to t
hem
. H
op
efu
lly
they
now
have
a m
ore
rob
ust
pro
du
ct.
92
.
En
de
(no s
peaker)
[Th
an
ks
for
the i
nte
rvie
w]
93
.
C Transcription of Interviews
110
Nik
ola
i_110525
Inte
rvie
w m
it D
r. N
ikola
i K
iese
l vo
m 2
5.0
5.2
01
1T
ran
scri
bed
by
yott
a,
vers
ion
1 o
f 1
10
52
6
An
fan
g,
pers
ön
lich
e D
ate
n,
Au
sbil
du
ng
Rein
hard
Zu
Beg
inn
wil
l ic
h e
igen
tlic
h e
h n
ur
all
gem
ein
e F
rag
en
ste
llen
. W
ie a
lt b
ist
du
?1
.N
ikola
i3
4.
2.
Rein
hard
Kan
nst
du
ku
rz s
chil
dern
: d
ein
Stu
diu
m,
dein
en
Werd
eg
an
g.
Wo d
u s
tud
iert
hast
?3
.N
ikola
iIc
h b
in z
um
stu
die
ren
nach
Mü
nch
en
geg
an
gen
. Ic
h k
om
me a
us
Nord
baye
rn,
au
sF
ran
ken
. In
der
Sch
ule
war
eig
en
tlic
h n
ich
t kla
r ob
ich
jetz
t C
hem
ie,
Ph
ysik
od
er
Math
e s
tud
iere
. U
nd
dan
n h
ab
e i
ch M
ath
e u
nd
Ph
ysik
an
gefa
ng
en
un
d b
in b
ei
der
Ph
ysik
hän
gen
geb
lieb
en
. N
ach
den
Lect
ure
s vo
n F
eyn
man
, als
o n
ach
dem
Bu
ch.
Dan
n h
ab
e i
ch i
n M
ün
chen
Ph
ysik
stu
die
rt.
Un
d h
ab
e e
igen
tlic
h e
rst
geg
en
En
de
dan
n i
n e
inem
Sem
inar
mit
gekri
eg
t vo
n d
en
exp
eri
men
tell
en
Sach
en
zu
rQ
uan
ten
ph
ysik
; vo
n H
ara
ld W
ein
furt
er
dort
. D
er
au
ch b
eim
An
ton
Zeil
ing
er
war.
Das
war
gan
z sp
an
nen
d u
nd
dan
n h
ab
e i
ch m
ir d
as
an
gesc
hau
t. U
nd
eh
er
noch
so
theore
tisc
he S
ach
en
zu
r S
up
ers
trin
gth
eori
e.
Ich
hab
e m
it i
n d
en
Url
au
bg
en
om
men
, d
ie p
ap
ers
. Fan
d i
ch d
an
n d
ie E
xperi
men
te d
er
Qu
an
ten
ph
ysik
doch
span
nen
der.
Dan
n w
ar
ich
dort
zu
r D
iplo
marb
eit
un
d d
an
n n
ach
ein
em
halb
en
Jah
rPau
se,
dan
n a
uch
zu
r D
okto
rarb
eit
.
4.
Rein
hard
Üb
er
was
die
Dip
lom
arb
eit
?5
.N
ikola
iD
as
war
Dre
i-P
hoto
nen
Vers
chrä
nku
ng
. Ic
h h
att
e e
inen
exp
eri
men
tell
en
Au
fbau
zu
ein
er
best
imm
ten
Art
von
Dre
i-P
hoto
nen
Vers
chrä
nku
ng
. A
lso W
-Sta
te,
imG
eg
en
satz
zu
dem
GH
Z-Z
ust
an
d [
Gre
en
berg
er,
Horn
e u
nd
Zeil
ing
er]
der
da [
inW
ien
] sc
hon
gem
ach
t w
ar.
Dan
n w
ar
ich
ein
halb
es
Jah
r w
eg
un
d b
in d
an
n a
uch
wie
der
in M
ult
i-P
hoto
nen
Vers
chrä
nku
ng
. A
lso d
an
n v
ier
Ph
oto
nen
.
6.
Rein
hard
Ja,
man
mu
ss s
ich
ste
igern
.7
.N
ikola
iG
en
au
, g
en
au
. A
uch
ein
ige m
eh
rere
Zu
stän
de.
Dan
n z
ur
Dokto
rarb
eit
geb
lieb
en
un
d d
an
n n
och
ein
Jah
r als
Post
-Doc.
Un
d d
an
n b
in i
ch h
ierh
er
geg
an
gen
zu
mM
ark
us
[Mark
us
Asp
elm
eye
r].
8.
Rein
hard
Das
war
jetz
t vo
r zw
ei
Jah
ren
, od
er?
9.
Nik
ola
iD
as
war
vor
zweie
inh
alb
Jah
ren
. W
eil
dan
n w
ar
es
mal
Zeit
irg
en
dw
ie t
hem
ati
sch
leic
ht
zu w
ech
seln
. A
lso e
s is
t im
mer
noch
natü
rlic
h e
xperi
men
tell
eQ
uan
ten
ph
ysik
, zu
min
dest
wü
nsc
hen
wir
un
s d
as
jetz
t h
ier.
Ab
er
halt
doch
ein
bis
serl
ein
an
dere
s S
yste
m,
un
d a
nd
ere
Hera
ng
eh
en
sweis
e,
neu
e M
eth
od
en
.
10
.
Rein
hard
Als
o a
uch
die
Moti
vati
on
wie
der
etw
as
neu
es
zu m
ach
en
?1
1.
Un
d w
ie b
ist
du
dan
n a
uf
hie
r g
ekom
men
?1
2.
Nik
ola
iIc
h h
ab
e m
ich
so e
in b
issc
hen
um
gesc
hau
t. E
s w
ar
kla
r d
as
es
Qu
an
ten
ph
ysik
sein
soll
. E
s w
ar
kla
r d
as
es
zum
ind
est
ein
bis
sch
en
Gru
nd
lag
en
sein
soll
en
. Ic
h w
oll
ten
ach
Mög
lich
keit
irg
en
dw
ie m
it m
ein
em
Wis
sen
um
gru
nd
leg
en
de S
ach
en
...
Als
om
it P
hoto
nen
kan
n m
an
halt
all
es
mög
lich
e s
chon
mach
en
, w
eil
sie
so e
infa
ch z
uh
an
dle
'n s
ind
. W
as
man
nic
ht
so r
ich
tig
lern
t si
nd
natü
rlic
h d
ie g
an
zen
Meth
od
en
die
an
kom
pli
ziert
ere
n E
xperi
men
ten
sta
ttfi
nd
en
. U
nd
ich
woll
te h
alt
das
irg
en
wie
kom
bin
iere
n.
Das
ich
die
an
dere
n M
eth
od
en
lern
e,
ab
er
da m
ein
Wis
sen
ein
bri
ng
e.
Weil
vie
le G
rup
pen
- d
as
wir
d jetz
t im
mer
wen
iger
- h
att
en
nic
ht
so A
hn
un
g v
or
ein
iger
Zeit
noch
. W
en
n m
an
jetz
t Q
ub
its
[Zw
eiz
ust
an
ds-
Qu
an
ten
syst
em
, an
alo
gzu
m k
lass
ich
en
Bit
in
der
Info
rmati
k]
hat,
was
man
da m
ach
en
kan
n;
au
ßer
Qu
an
ten
info
rmati
on
.
13
.
Rein
hard
Als
o d
as
es
da a
uf
dem
Leve
l st
eh
en
geb
lieb
en
ist
, od
er?
14
.N
ikola
iJa
. D
as
kam
halt
meis
ten
s vo
n d
er
Sach
e h
er,
jetz
t zu
m B
eis
pie
l S
up
erc
on
du
ctin
gQ
ub
its.
Das
kam
halt
meis
ten
s vo
n d
er
Sach
e h
er:
Ja,
jetz
t h
at
man
ein
Sys
tem
.Q
uan
ten
info
rmati
on
ist
irg
en
dw
ie c
ool
un
d d
esw
eg
en
ist
Qu
bit
s to
ll.
Un
d jetz
tm
ach
t m
an
so Q
ub
its
un
d n
atü
rlic
h w
ill
man
vie
le.
Un
d m
an
wil
l d
as
inte
gri
ert
fü
rein
en
Qu
an
ten
com
pu
ter.
Ab
er
das
es
jetz
t d
a e
ine g
an
ze W
elt
- a
lso v
iell
eic
ht
un
ters
tell
e i
ch d
as
au
ch n
ur
- vo
n T
heori
e z
ur
Vers
chrä
nku
ng
gib
t u
nd
das
man
nic
ht
imm
er
nu
r ein
e B
ell
Un
gle
ich
un
g m
ess
en
mu
ss,
wen
n m
an
Vers
chrä
nku
ng
nach
weis
en
wil
l; z
um
Beis
pie
l. D
as
ware
n S
ach
en
die
jetz
t ers
t so
mit
der
Zeit
so
rich
tig
bekan
nt
werd
en
; g
lau
be i
ch.
15
.
Au
fgab
e i
m E
xp
eri
men
t /
Roll
e i
n d
er
Gru
pp
e
Rein
hard
Was
ist
da s
o d
ein
e R
oll
e i
n G
rup
pe?
Ich
weiß
, d
ass
du
das
Exp
eri
men
t m
it d
en
"Ku
gerl
n",
od
er.
..1
6.
Nik
ola
iM
it d
en
Nan
oku
geln
.1
7.
Rein
hard
Kli
ng
t ein
bis
sch
en
pro
fess
ion
ell
er.
18
.N
ikola
iN
an
o-K
ug
eln
ist
au
ch n
ich
t so
pro
fess
ion
ell
. Ja
, als
ich
vor
zweie
inh
alb
Jah
ren
kam
in d
ie G
rup
pe,
da h
ab
e i
ch e
igen
tlic
h n
och
so e
in b
issc
hen
mit
gearb
eit
et
am
Exp
eri
men
t, a
n d
em
jetz
t au
ch W
itle
f [W
itle
f W
iecz
ore
k]
ist,
mit
den
can
tile
vern
.H
ab
e m
ich
hau
pts
äch
lich
...
Als
o i
ch b
in ja i
m R
ah
men
von
ein
em
Hu
mb
old
t-S
tip
en
dia
t h
ier.
Das
gin
g i
m w
ese
ntl
ich
um
Ein
zel-
Ph
oto
nen
Qu
an
ten
-O
pto
mech
an
ik u
nd
Vers
chrä
nku
ng
. W
ie s
o o
ft i
n s
olc
hen
Sach
en
zie
ht
sich
das
halt
län
ger
hin
. U
nd
so z
ur
halb
en
Zeit
, od
er
sow
as,
kam
dan
n d
iese
s...
Als
o v
or
ein
ein
halb
Jah
ren
fast
jetz
t, k
am
dan
n d
iese
Sach
e a
uf
mit
den
Nan
oku
geln
. U
nd
da b
in i
ch d
an
n a
ufg
esp
run
gen
. A
ls i
ch k
am
war
die
Gru
pp
e n
och
nic
ht
so r
iesi
g.
Da w
are
n w
ir i
rgen
dw
ie z
u f
ün
ft;
gla
ub
e i
ch.
In d
er
Zw
isch
en
zeit
, d
urc
h d
en
Ru
fvo
m M
ark
us
[Mark
us
Asp
elm
eye
r],
sin
d w
ird
jetz
t h
alt
noch
zw
ei
meh
r Post
-Docs
un
d n
och
ein
paar
Leu
te.
Ich
ble
ibe a
uch
noch
län
ger
da.
19
.
Rein
hard
Ein
e g
röß
ere
Pla
nu
ng
? A
lso s
chon
weit
er
gep
lan
t, w
as
du
mach
en
wil
lst?
20
.N
ikola
iG
en
au
. A
lso d
as
Exp
eri
men
t w
erd
e i
ch jetz
t w
eit
er
mit
au
sbau
en
. U
nd
bin
ich
natü
rlic
h a
uch
bei
den
gan
zen
Nic
ht-
exp
eri
men
tell
en
Sach
en
so m
itb
ete
ilig
t. W
as
21
.
111
halt
im
mer
dam
it z
u t
un
hat?
Was
man
halt
so m
it d
er
Zeit
au
ch m
ach
t.R
ein
hard
Un
d d
as
wäre
?2
2.
Nik
ola
iN
aja
. D
as
sin
d h
alt
so S
ach
en
, w
ie w
en
n e
s u
m i
rgen
dw
elc
he V
era
nts
talt
un
gen
geh
t. A
lso w
as
halt
mit
der
Zeit
au
f ein
en
zu
kom
mt,
wen
n m
an
dan
n m
al
irg
en
dw
an
n s
elb
er
sow
eit
ist
, w
ie d
er
Mark
us
[Mark
us
Asp
elm
eye
r].
Dan
n k
om
mt
man
eh
nic
ht
meh
r in
s L
ab
or.
Im
Mom
en
t b
in i
ch n
och
vie
l im
Lab
or;
das
ist
gu
t.
23
.
Rein
hard
Wie
ist
den
n u
ng
efä
hr
der
Sta
tus
im E
xperi
men
t?2
4.
Nik
ola
iD
er
Sta
tus
im E
xperi
men
t [L
ach
en
]. D
er
än
dert
sic
h t
äg
lich
. D
as
Exp
eri
men
t sa
ham
An
fan
g w
ie i
mm
er
gan
z ein
fach
au
s. D
a w
ar
es
au
ch s
o,
dass
es.
.. E
s is
t im
mer
noch
was
gan
z n
eu
es.
Es
hat
in d
iese
r F
orm
bis
jetz
t n
och
kein
er
levi
tiert
eN
an
o-K
ug
eln
in
Cavi
ty-O
pto
-Mech
an
ik v
erw
en
det.
Dad
urc
h s
oll
te d
as
ja a
uch
sch
nell
geh
en
, d
am
it e
s n
iem
an
d a
nd
ers
vor
un
s m
ach
t; g
an
z kla
r. A
ber
es
ist
gan
zkla
r, d
ass
die
Moti
vati
on
von
dem
Exp
eri
men
t n
atü
rlic
h i
st,
irg
en
dw
an
n g
ute
Qu
an
ten
ph
ysik
zu
mach
en
. W
eil
levi
tiert
e K
ug
eln
su
per
geeig
net
sin
d.
25
.
Der
Sta
tus
im E
xperi
men
t is
t d
er:
Mit
der
Zeit
fin
det
man
dan
n r
au
s w
o e
s h
akt.
Un
d w
ir h
att
en
dan
n i
m w
ese
ntl
ich
en
all
es
dast
eh
en
. N
ur
un
sere
Ku
geln
die
bra
uch
en
wir
ja b
ei
tiefe
m V
aku
um
. U
nd
ein
e S
ach
e d
ie n
ich
t kla
r is
t, w
aru
m w
irn
ich
t in
s ti
efe
Vaku
um
kön
nen
. W
eil
die
Ku
geln
geh
en
vorh
er
verl
ore
n.
Die
ble
iben
nic
ht
in d
er
Fall
e.
Bei
ein
bis
sch
en
un
ter
ein
em
Mil
lib
ar
vers
chw
ind
en
die
. D
as
ist
ein
e S
ach
e,
die
jetz
t so
ist
. Ja
, g
ar
nic
ht
qu
an
ten
mech
an
isch
, n
ur
an
stre
ng
en
d.
Au
fd
er
an
dere
n S
eit
e i
st e
s so
, d
ass
wir
natü
rlic
h d
ie C
avi
ty-O
pto
-Mech
an
ik s
eh
en
woll
en
un
d d
a i
st e
s in
letz
ter
Zeit
zie
mli
ch g
ut
geg
an
gen
. W
ir s
eh
en
jetz
t ein
Sig
nal
in d
er
cavi
ty u
nd
dam
it k
ön
nen
wir
jetz
t d
ie e
rste
n M
eth
od
en
zeig
en
. U
nd
zeig
en
, p
roof-
of-
pri
nci
ple
, d
ass
wen
n m
an
den
n m
al
zu e
inem
nie
dri
gere
m D
ruck
kom
mt,
dass
man
dan
n a
uch
ein
Gro
un
d-S
tate
-Cooli
ng
[d
.h.
das
Sys
tem
in
den
Gru
nd
zust
an
d=
Qu
an
ten
zust
an
d z
u b
rin
gen
] u
nd
so m
ach
en
kan
n. In
sofe
rn i
st d
as
ein
gu
ter
Zeit
pu
nkt
die
Fra
ge z
u s
tell
en
.
26
.
Rein
hard
Die
best
e Z
eit
ist
wah
rsch
ein
lich
, w
en
n m
an
das
voll
e E
rgeb
nis
hat
un
d s
chon
all
ep
ap
ers
rau
s. D
as
ist
der
best
e S
tatu
s vo
m E
xperi
men
t.2
7.
Nik
ola
iIc
h g
lau
be d
er
best
e S
tatu
s is
t in
dem
Mom
en
t w
o m
an
weiß
was
man
jetz
tau
fsch
reib
en
kan
n.
Weil
wen
n d
ie p
ap
er.
.. d
an
n w
ird
es
sch
on
wie
der
an
stre
ng
en
d.
28
.
Rein
hard
Un
d b
ei
dem
Exp
eri
men
t w
ars
t d
u v
on
An
fan
g a
n d
ab
ei?
D.h
. au
ch i
n d
er
Kon
zip
ieru
ng
un
d t
heore
tisc
hen
En
twic
klu
ng
?2
9.
Nik
ola
iJa
, d
as
hab
e i
ch a
ufg
ezo
gen
. E
s g
ab
ein
Th
eori
e-P
ap
er
davo
r; a
lso v
on
an
dere
nG
rup
pen
. U
nd
da a
rbeit
en
wir
au
ch m
it e
iner
zusa
mm
en
; m
it d
er
Ign
aci
o C
irac
[Gru
pp
e]
in M
ün
chen
. A
ber
all
es
was
das
Exp
eri
men
tell
e b
etr
ifft
un
d w
ie w
ir e
sau
fbau
en
, h
ab
e i
ch d
an
n a
ng
efa
ng
en
. U
nd
dan
n k
am
ein
Dp
lom
an
d d
azu
un
d d
an
nsp
äte
r n
och
Flo
rian
[F
lori
an
Bla
ser]
als
Dokto
ran
d.
Jetz
t m
ach
en
wir
das
som
itein
an
der.
30
.
Fasz
inati
on
an
der
Qu
an
ten
mech
an
ik
Rein
hard
Jetz
t zu
etw
as
an
dere
m.
Was
wü
rdest
du
als
fasz
inie
ren
stes
Featu
re s
eh
en
, je
tzt
31
.
von
der
Qu
an
ten
mech
an
ik?
Was
dic
h b
eg
eis
tert
in
die
sem
Feld
? W
as
ein
en
moti
viert
?N
ikola
iD
as
hat
viele
Asp
ekte
. E
in H
au
pta
spekt
ist
der,
dass
die
se A
ha-E
rleb
nis
se n
ich
tau
fhöre
n.
Als
o i
ch h
ab
e jetz
t...
Wir
hab
en
letz
ten
s d
ie D
isku
ssio
n g
eh
ab
t. I
ch h
ab
ein
mein
er
Dip
lom
arb
eit
eb
en
au
ch m
it B
ell
Un
gle
ich
un
gen
un
d s
o s
chon
zu
tu
ng
eh
ab
t. A
lso d
as
"kla
ssis
che"
Beis
pie
l im
qu
an
ten
mech
an
isch
en
Kon
text
. U
nd
trotz
dem
mu
ss m
an
es
imm
er
noch
mal
von
ein
er
an
dere
n S
eit
e a
nsc
hau
en
. U
nd
trotz
dem
mu
ss m
an
noch
mal
vers
teh
en
was
da p
ass
iert
. Ic
h g
lau
be d
as
ist
das
Fasz
inie
ren
de.
Dad
urc
h d
as
man
es
nic
ht
dir
ekt
gre
ifen
kan
n,
was
den
n jetz
t d
ieQ
uan
ten
ph
ysik
au
smach
t. U
nd
wie
man
es
jetz
t ri
chti
g s
ag
t. D
ad
urc
h m
uss
man
so
viele
vers
chie
den
e M
od
ell
e i
m K
op
f en
twic
keln
. A
lso i
ch w
eiß
bei
mir
pers
ön
lich
,d
ass
was
mir
am
meis
ten
Sp
aß
mach
t -
üb
erh
au
pt
an
der
Ph
ysik
- i
mm
er
die
Sic
htw
eis
e z
un
än
dern
. Ic
h g
lau
be,
dass
das
eh
er
ein
all
gem
ein
es
Ph
än
om
en
ist
.
32
.
An
dere
rseit
s, e
s kli
ng
t kom
isch
, ab
er
was
natü
rlic
h i
rgen
dw
ie t
oll
war,
gera
de i
nd
er
Zeit
der
Dip
lom
arb
eit
- d
as
ist
jetz
t m
it d
en
Exp
eri
men
ten
die
wir
jetz
t m
ach
en
ein
bis
sch
en
an
ders
-..
. D
iese
Qu
bit
Rech
nere
i is
t ja
rela
tiv
ein
fach
zu
gän
gli
ch.
Das
war
ein
Geb
iet
in d
em
man
rela
tiv
sch
nell
ein
steig
en
kon
nte
Sach
en
zu
mach
en
,d
ie jetz
t si
ch n
och
nie
man
d s
o ü
berl
eg
t h
att
e.
Od
er
man
neu
e I
deen
hab
en
kon
nte
,oh
ne d
as
man
wir
kli
ch e
in r
iesi
ges
Fu
nd
am
en
t vo
n W
isse
n g
eb
rau
cht
hätt
e.
Das
ist
natü
rlic
h m
it d
en
Exp
eri
men
ten
wie
es
jetz
t h
ier
ist,
od
er
was
wir
au
ch p
lan
en
wir
kli
ch Q
uan
ten
ph
ysik
dam
it z
u m
ach
en
, n
ich
t m
eh
r g
an
z so
ein
fach
.
33
.
Rein
hard
Ab
er
sch
ein
t h
alt
mit
der
Zeit
meh
r zu
werd
en
. E
s w
ird
ja i
mm
er
meh
r Tech
nik
rein
gest
eck
t. O
der
Din
ge d
ie d
u d
an
n z
usä
tzli
ch b
rau
chst
. W
ie d
u s
chon
gesa
gt
hast
, n
ich
t m
eh
r so
ein
fach
wie
die
Bell
Exp
eri
men
te s
ind
.
34
.
Nik
ola
iE
s w
ird
au
ch k
on
zep
tion
ell
sch
wie
rig
er.
Wen
n m
an
jetz
t g
era
de s
ieh
t h
ier
bei
un
sm
it m
ass
iven
Ob
jekte
n g
eh
t n
atü
rlic
h i
n e
inen
Bere
ich
wo e
s an
Gra
vita
tion
stö
sst.
Da w
oll
en
wir
ja a
uch
hin
. D
as
verl
an
gt
natü
rlic
h a
uch
, d
ass
man
sic
h d
as
zusä
tzli
che W
isse
n a
neig
net.
Was
ja S
inn
un
d Z
weck
der
Üb
un
g i
st.
Als
o,
in a
nu
tsh
ell
: D
as
Fasz
inie
ren
dst
e f
ür
mic
h i
st d
as.
.. M
an
kan
n e
s n
ich
t d
irekt
beg
reif
en
, d
esw
eg
en
mu
ss m
an
so v
iele
Pers
pekti
ven
fin
den
au
s d
en
en
man
es
besc
hre
iben
kan
n.
35
.
Inte
rpre
tati
on
/ T
heori
e /
Exp
eri
men
t
Rein
hard
Ab
er
das
treib
t d
as
Din
g a
uch
irg
en
dw
ie w
eit
er.
Das
mach
t ja
dan
n a
uch
die
Moti
vati
on
fü
r E
xperi
men
te a
us.
Wen
n m
an
eb
en
nic
ht
gan
z si
cher
ist
au
f w
as
das
hin
au
släu
ft.
Ob
das
Exp
eri
men
t so
jetz
t fu
nkti
on
iert
, od
er
ob
man
nic
ht
au
f n
eu
es
stöß
t?
36
.
Nik
ola
iE
iners
eit
s ü
berh
au
pt
au
f g
an
z n
eu
es
stöß
t. A
nd
ere
rseit
s -
das
kli
ng
t fa
stab
wert
en
d z
um
Exp
eri
men
t is
t ab
er
gar
nic
ht
so g
em
ein
t, i
m G
eg
en
teil
- i
st e
sn
atü
rlic
h e
ine A
rt s
ich
dam
it z
u b
esc
häft
igen
, d
ie e
inen
zw
ing
t S
ach
en
dan
n h
alt
rich
tig
zu
seh
en
. D
an
n d
en
kt
man
darü
ber
nach
un
d d
en
kt
das
mü
sste
so u
nd
so
sein
. Is
t es
dan
n e
ben
jetz
t n
ich
t so
, n
ich
t w
eil
die
Th
eori
e i
rgen
dw
ie g
eän
dert
werd
en
mü
sste
, so
nd
ern
ein
fach
weil
man
noch
ein
en
Kn
ote
n i
m H
irn
hat.
Es
ist
ein
e A
rt d
am
it z
u s
pie
len
. W
en
n m
an
rech
t n
ett
ist
, ein
e a
nd
ere
Art
dam
it z
usp
iele
n.
37
.
Rein
hard
Wie
wü
rdest
du
dan
n d
ie B
ezi
eh
un
g s
o v
on
Th
eori
e u
nd
Exp
eri
men
t se
hen
? W
eil
es
38
.
C Transcription of Interviews
112
ja s
chw
ieri
g i
st.
Th
eori
e u
nd
Exp
eri
men
t g
eh
t ja
dan
n n
och
, ab
er
wen
n m
an
dan
nso
an
In
terp
reta
tion
en
den
kt.
Die
sp
iele
n d
an
n i
m E
xperi
men
t d
an
n k
au
m e
ine
Roll
e?
Nik
ola
iIn
dem
Mom
en
t w
o m
an
am
Exp
eri
men
t st
eh
t h
at
man
ja i
mm
er
mit
kla
ssic
hen
Gerä
ten
zu
tu
n.
Da w
o e
s ab
er
sch
on
au
f ein
e A
rt,
man
chm
al,
selt
en
rein
kom
mt
ist
natü
rlic
h w
en
n m
an
dan
n..
. M
an
mu
ss ja n
ich
t n
ur
üb
erl
eg
en
jetz
t: I
ch w
eiß
jetz
tw
ie i
ch d
as
mach
e u
nd
dan
n s
eh
e i
ch d
as
am
Sch
luß
, od
er
was
seh
e i
ch d
an
n a
mS
chlu
ß.
Son
dern
jetz
t is
t d
as
all
es
nic
ht
so w
ie i
ch e
s w
ill,
kan
n i
ch t
rotz
dem
ein
en
Eff
ekt
seh
en
. U
nd
in
dem
Mom
en
t m
uss
man
natü
rlic
h w
ied
er
darü
ber
nach
den
ken
. U
nd
sie
ht
viell
eic
ht
was
neu
es,
was
ein
em
nic
ht
vorh
er
kla
r w
ar,
dass
da i
st.
Ab
er
das
ist
tats
äch
lich
, g
lau
be i
ch,
das
Ein
zig
e w
o d
as
Exp
eri
men
t...
Wen
nm
an
nic
ht
die
ric
hti
gen
Bil
der
im K
op
f h
at,
dan
n h
at
man
au
ch n
ich
t d
ie r
ich
tig
eId
ee w
ie m
an
das
mach
t.
39
.
Rein
hard
Vers
teh
e.
Un
d i
st e
s ir
gen
dw
ie p
ers
ön
lich
in
tere
ssan
t fü
r d
ich
die
se S
ach
en
... S
ind
die
rele
van
t, I
nte
rpre
taio
nen
, d
ie e
s d
a,
wen
n m
an
wil
l au
ch "
kla
ssis
ch"
nen
nen
[kön
nte
], g
ibt?
Fall
s m
an
sie
üb
erh
au
pt
mit
bekom
mt?
D.h
. w
as
man
im
Stu
diu
mle
rnt,
bzw
. w
as
du
gele
rnt
hast
?
40
.
Nik
ola
iN
och
mal?
Ich
hab
e d
as
nic
ht
gan
z ve
rsta
nd
en
.4
1.
Rein
hard
Nein
, ob
so p
rin
zip
iell
e F
rag
en
, w
ie jetz
t ein
e I
nte
rpre
tati
on
wie
die
Kop
en
hag
en
er
Deu
tun
g o
der
Boh
msc
he M
ech
an
ik,
Vie
l-W
elt
en
Th
eori
en
un
d w
as
da s
oh
eru
msc
hw
irrt
. E
iners
eit
s ob
man
das
üb
erh
au
pt
im S
tud
ium
irg
en
dw
iem
itb
ekom
mt.
Un
d o
b d
as
üb
erh
au
pt
ein
e R
oll
e s
pie
lt?
42
.
Nik
ola
iIm
Stu
diu
m m
itb
ekom
mt?
Ja.
Als
o i
ch h
ab
e i
m S
tud
ium
sch
on
ein
bis
sch
en
was
mit
bekom
men
. W
as
zum
Teil
dara
n l
ag
, d
ass
es
halt
, zu
m B
eis
pie
l, s
o e
inen
Boh
m'ian
er
an
der
LM
U [
Lu
dw
ig-M
axi
mil
ian
s-U
niv
ers
ität
Mü
nch
en
] g
ibt.
Der
hatt
e e
ine M
ath
e V
orl
esu
ng
, d
ie e
ine v
ers
teck
te B
oh
m V
orl
esu
ng
war.
43
.
Rein
hard
Mu
sste
er
sich
vers
teck
en
?4
4.
Nik
ola
iJa
, es
ist
sch
on
...
Ich
gla
ub
e d
er
hat
ein
en
hart
en
Sta
nd
da.
Als
o d
as
ist
all
es
seh
rkon
serv
ati
ves
Um
feld
. W
en
n m
an
so w
ill,
qu
an
ten
mech
an
isch
kon
serv
ati
ves
Um
feld
.
45
.
Rein
hard
Da i
st e
s eb
en
die
Fra
ge,
was
da n
och
du
rch
sch
ein
t? O
der
ob
du
nu
r d
en
norm
ale
nq
uan
ten
mech
an
isch
en
Leh
rpla
n h
ast
? D
er
eh
zie
mli
ch g
leic
h i
st ü
bera
ll.
46
.
Nik
ola
iN
ein
, in
der
Form
wie
ich
es
jetz
t g
esa
gt
hab
e,
hat
man
das
sch
on
mit
gekri
eg
t. O
bic
h e
s je
tzt
halt
noch
so s
eh
en
wü
rde,
ob
das
so i
st o
der
ob
das
nu
r so
verm
itte
lt[w
urd
e],
weiß
ich
nic
ht.
Ab
er
mir
kam
das
dam
als
so v
or:
Ja,
der
hat
jetz
t d
iese
an
dere
In
terp
reta
tion
. D
er
hat
das
au
ch m
it F
eu
ere
ifer
vers
uch
t kla
r zu
mach
en
,d
ass
das
die
bess
ere
Sic
htw
eis
e i
st.
Un
d d
as
er
da a
ng
eeck
t is
t, d
as
war
au
chall
seit
s b
ekan
nt.
In
sofe
rn w
ar
das
au
ch i
nte
ress
an
t. A
lso i
ch w
ar,
das
hän
gt
jaim
mer
viel
davo
n a
b,
mit
vie
len
Leu
ten
mit
den
en
man
dan
n ü
ber
die
se S
ach
en
gere
det
hat
beie
inan
der.
Au
ch B
ell
un
d s
o w
eit
er.
Was
bed
eu
tet
es
un
d w
ie k
an
nm
an
es
vers
teh
en
. R
ele
van
t? J
a,
es
ist
für
mic
h h
au
pts
äch
lich
rele
van
t, w
eil
es
ein
evo
n d
en
Sach
en
ist
, d
ie m
ich
am
meis
ten
in
tere
ssie
ren
. Ic
h g
lau
be i
ch k
ön
nte
, d
ass
was
ich
jetz
t m
ach
e g
en
au
so m
ach
en
, w
en
n i
ch d
as
jetz
t n
ich
t so
wü
sste
all
es.
Ab
er
gera
de w
en
n e
inen
das
inte
ress
iert
ist
hie
r d
as
rich
tig
e U
mfe
ld,
gla
ub
e i
ch.
47
.
Rein
hard
Die
Fra
ge i
st a
uch
ob
in
wie
weit
ein
en
sow
as
zum
ind
est
hil
ft b
ess
er
zu v
ers
teh
en
?O
der
zum
ind
est
, w
en
n m
an
meh
rere
Sic
htw
eis
en
hat,
zu
m B
eis
pie
l d
ie B
oh
m's
che
so d
an
eb
en
ste
llt,
im
Verg
leic
h e
in b
ess
ere
s G
efü
hl
bekom
mt?
Wie
die
Sach
e l
ieg
t,od
er
was
die
ein
e e
rklä
rt,
was
die
an
dere
sch
wie
rig
er
erk
lärt
?
48
.
Nik
ola
iIc
h m
uss
dazu
sag
en
jetz
t...
Es
ist
ein
ext
rem
un
ters
chie
dli
ches
Leve
l au
f d
em
ich
die
se S
ach
en
un
ters
chie
dli
ch k
en
ne.
Bei
Boh
m jetz
t zu
m B
eis
pie
l kan
n i
ch n
ich
tvi
el
dazu
sag
en
, d
a g
ibt
es
nu
r zw
ei,
dre
i B
ild
er
im K
op
f. A
uf
ein
em
Vers
tän
dn
is-L
eve
l h
ilft
es.
Als
o a
uf
ein
em
ein
fach
th
eore
tisc
hen
Leve
l h
ilft
es
ein
fach
deh
alb
, w
eil
wen
n m
an
was
au
ch a
nd
ere
s ve
rste
hen
kan
n,
dan
n m
uss
man
sich
fra
gen
waru
m m
an
es
so u
nd
nic
ht
an
ders
mein
t. A
uf
dem
Leve
l, ja.
Wie
gesa
gt
für
die
kon
kre
te A
rbeit
, n
ein
. A
lso i
ch g
lau
be,
dass
...
Kon
kre
te A
rbeit
mein
eic
h jetz
t L
ab
ora
rbeit
, ab
er
natü
rlic
h i
st e
s Teil
der
Arb
eit
. D
en
n w
ir d
isku
tiere
n ja
hie
r st
än
dig
üb
er
solc
he S
ach
en
.
49
.
Rein
hard
Ab
er
das
sch
ein
t au
ch e
ine M
ög
lich
keit
zu
sein
, zu
min
dest
in
der
Besc
häft
igu
ng
dam
it,
das
Vers
tän
dn
is z
u s
teig
ern
. D
as
wil
l m
an
ja z
um
ind
est
, d
ass
man
Din
ge
bess
er
vers
teh
t. U
nd
das
ist
au
ch f
ür
dic
h e
in M
itte
l d
as
bess
er
zu v
ers
teh
en
?
50
.
Nik
ola
iJa
, ja
. A
uf
jed
en
Fall
.5
1.
tech
nis
ch
er
Fort
sch
ritt
Rein
hard
Ein
e F
rag
e i
st n
och
in
wie
weit
wü
rdest
du
das
ein
sch
ätz
en
, w
ie s
ich
du
rch
tech
nis
che M
ög
lich
keit
en
eb
en
die
Mög
lich
keit
en
im
Bere
ich
der
exp
eri
men
tell
en
Qu
an
ten
mech
an
ik a
usw
irken
? W
eil
es
sch
ein
t ja
doch
ein
, m
uss
man
sch
on
sag
en
ein
paar
Jah
re o
der
man
kan
n s
chon
bald
Jah
rzeh
nte
sag
en
...
dass
es
da d
och
ein
en
zie
mli
chen
An
sch
ub
gib
t, w
en
n m
an
vie
lleic
ht
die
vorh
eri
gen
Peri
od
en
verg
leic
ht.
52
.
Nik
ola
iJa
, d
a i
st p
lötz
lich
vie
l p
ass
iert
in
ku
rzer
Zeit
. S
pezi
ell
der
tech
nis
che A
spekt
ist
gera
de jetz
t m
it d
er
Op
to-M
ech
an
ik s
o,
dass
ein
fach
vor
zeh
n J
ah
ren
die
Tech
nolo
gie
nic
ht
da w
ar
um
die
Exp
eri
men
te z
u m
ach
en
. D
as
kan
n m
an
sch
lich
tu
nd
erg
reif
en
d s
o s
ag
en
. D
a g
ab
es
natü
rlic
h d
ie I
deen
das
zu m
ach
en
un
d a
uch
Leu
te,
die
das
an
gefa
ng
en
hab
en
. A
ber
die
Tech
nolo
gie
das
so z
u m
ach
en
ist
jetz
ters
t d
a.
Vie
le S
yste
me w
erd
en
natü
rlic
h e
rst
so e
ntw
ickelt
, ab
er
die
Meth
od
en
sin
d e
rst
da.
Von
dah
er
hat
es
ein
en
rie
sig
en
Ein
flu
ß.
Das
gil
t je
tzt
hau
pts
äch
lich
für
die
Exp
eri
men
te [
hie
r in
die
ser
Gru
pp
e].
Wen
n m
an
die
Ph
oto
nen
exp
eri
men
tean
sch
au
t is
t m
ir n
ich
t g
an
z kla
r w
aru
m d
as
an
ein
er
Ste
lle s
o e
inen
Sch
ub
gab
.W
eil
das
hätt
e m
an
au
ch v
orh
er,
wen
n m
an
es
gep
ush
t h
ätt
e,
viell
eic
ht
frü
her.
..A
ber
da b
rau
chts
halt
dan
n n
och
die
Leu
te,
die
das
mach
en
ein
fach
.
53
.
Rein
hard
Es
hat
sich
sic
her
au
ch M
oti
vati
on
slag
e g
eän
dert
. Ir
gen
dw
ie g
ibt
es
ja d
en
Wu
nsc
hm
it d
em
was
an
zufa
ng
en
. A
nw
en
du
ng
en
zu
hab
en
. A
lso w
en
n i
ch d
ie S
chla
gw
ört
er
sag
e:
Qu
an
ten
com
pu
ter,
Kry
pto
gra
ph
ie u
nd
In
form
ati
on
stech
nik
...
54
.
Nik
ola
iS
ich
er
gib
t es
Leu
te,
die
gen
au
die
Vis
ion
hab
en
. W
ob
ei
gen
au
die
Ap
pli
kati
on
ssch
lag
wort
e n
atü
rlic
h s
chon
sta
rk g
etr
ieb
en
sin
d,
weil
man
sie
au
chfi
nan
ziere
n m
uss
. A
lso i
ch g
lau
be,
dass
, je
tzt
wen
iger,
ab
er
vor
all
em
in
der
Zeit
wo d
as
geb
oom
t h
at
am
An
fan
g.
Das
ist
vor
mein
er
wis
sen
sch
aft
lich
seh
r akti
ven
55
.
113
Zeit
, d
esw
eg
en
kan
n i
ch d
as
nu
r ra
ten
. A
ber
die
all
er
meis
ten
Leu
te,
die
was
gem
ach
t h
ab
en
, ers
tmal
gar
nic
ht
dara
n i
nte
ress
iert
ware
n A
nw
en
du
ng
en
zu
mach
en
. U
nd
das
halt
nu
r ein
e F
inan
zieru
ng
ssach
e w
ar.
Jetz
t w
o d
ie T
ech
nolo
gie
nw
eit
gen
ug
sin
d,
gib
t es
da e
inig
e d
ie d
a w
irkli
ch a
kti
v u
nd
erf
olg
reic
h d
ara
narb
eit
en
. A
ber
das
ist
meh
r so
, d
as
ist
jetz
t b
öse
gesa
gt,
ab
er
wen
n e
inem
was
bess
ere
s ein
fall
en
wü
rde w
as
Gru
nd
lag
en
ph
ysik
betr
ifft,
dan
n w
ürd
en
die
All
erm
eis
ten
das
lieb
er
mach
en
. A
ls jetz
t h
ier
bess
ere
Lase
r zu
bau
en
, d
ie d
an
nein
en
Qu
an
ten
com
pu
ter
erm
ög
lich
en
. D
er
Boom
ist
ers
tau
nli
ch,
der
dan
nir
gen
dw
an
n k
am
. D
as
inte
ress
an
t. H
än
gt
natü
rlic
h a
uch
mit
dem
zu
sam
men
, d
ass
dan
n G
eld
da w
ar
für
Qu
an
ten
com
pu
ter.
Rein
hard
Das
ist
es
ja a
uch
, d
ass
man
hie
r W
ach
stu
m s
ieh
t. A
uch
exp
eri
men
tell
. In
gew
isse
rW
eis
e s
chein
en
die
Th
eori
en
, zu
min
dest
der
math
em
ati
sch
e K
orp
us,
geg
eb
en
. D
ieG
run
dla
gen
au
f je
den
Fall
. F
ür
die
Mu
lti-
Ph
oto
nen
Vers
chrä
nku
ng
bra
uch
t m
an
viell
eic
ht
au
ch m
ath
em
ati
sch
meh
r. E
xperi
men
tell
gib
t es
noch
meh
rU
nen
tdeck
tes.
56
.
Nik
ola
iJa
, es
gib
t zu
min
dest
vie
l zu
tu
n.
Es
gib
t h
alt
vie
l zu
tu
n,
weil
wen
n m
an
an
Ap
pli
kati
on
en
den
kt
au
ch d
er
Tra
nsi
tor
noch
nic
ht
erf
un
den
ist
[A
nsp
ielu
ng
, d
ass
man
gern
e e
in Q
uan
ten
an
alo
gon
zu
m k
lass
ich
en
Tra
nsi
stor
fin
den
wü
rde]
inkein
er
von
den
gan
zen
Sys
tem
en
.
57
.
Au
sbli
ck /
mög
lich
e L
ösu
ng
?
Rein
hard
Sie
hst
du
eig
en
tlic
h e
ine M
ög
lich
keit
, d
ass
was
du
vorh
er
gesa
gt
hast
, d
ass
da
noch
etw
as
un
best
imm
t is
t od
er
dass
man
sic
h D
ing
e i
mm
er
noch
ein
mal
an
sch
au
en
mu
ss u
m s
ich
er
zu g
eh
en
, d
ass
man
sic
h a
uch
wir
kli
ch i
m B
ere
ich
der
Qu
an
ten
befi
nd
et,
dass
man
das
irg
en
dw
ie a
ufl
öse
n k
an
n?
Od
er
das
sich
da i
rgen
detw
as
erg
ibt?
Od
er,
dass
man
ein
e A
rt H
off
nu
ng
hat,
dass
irg
en
dw
an
n jem
an
d m
itein
er
Th
eori
e k
om
mt
die
ein
em
das
pla
usi
ble
r m
ach
t od
er
dir
ekt
zug
än
gli
cher?
Od
er
mu
ss e
s im
mer
off
en
, im
Wech
sels
pie
l, b
leib
en
?
58
.
Nik
ola
iIc
h d
en
ke,
dass
man
sic
h s
tark
dara
n a
np
ass
en
wir
d.
Vie
les
was
ein
em
jetz
tkom
isch
vork
om
mt.
.. D
as
ist
jetz
t ein
e s
eh
r su
bje
kti
ve M
ein
un
g.
Ab
er
es
ist
jair
gen
dw
ie n
ur
ein
e G
ew
oh
nh
eit
. W
ir h
att
en
kü
rzli
ch d
ie D
isku
ssio
n,
um
ein
kon
kre
tes
Beis
pie
l zu
sag
en
: M
ess
pro
ble
m u
nd
jetz
t sa
gt
man
irg
en
dw
o m
uss
ja
die
se W
ell
en
fun
kti
on
dan
n d
och
kola
bie
ren
. Ja
, w
aru
m e
igen
tlic
h.
Das
kön
nte
man
sich
ja v
ors
tell
en
: W
ir s
ind
halt
Teil
die
ser
gro
ßen
Well
en
fun
kti
on
. U
nd
wie
wir
halt
gera
de d
asi
tzen
ist
nu
r so
ein
e R
eali
sieru
ng
. D
afü
r b
rau
cht
man
au
ch n
ich
tV
iele
-Welt
en
, w
eil
Su
perp
osi
tion
. Pass
t sc
hon
. W
o i
st e
igen
tlic
h d
as
Pro
ble
m?
Es
ist
lust
ig,
weil
es
sin
d..
. Je
der
mit
dem
ich
hie
r re
de h
at
sich
au
sgie
big
st m
itQ
uan
ten
mech
an
ik a
use
inan
derg
ese
tzt.
Un
d v
iele
, ic
h g
lau
be d
ie a
lten
Hase
nw
ürd
en
eh
er
ein
e k
riti
sch
ere
An
twort
dara
uf
geb
en
kön
nen
, ab
er
viele
sag
en
: W
ois
t eig
en
tlic
h d
as
Pro
ble
m?
59
.
Ich
gla
ub
e,
dass
man
sic
h a
n S
ach
en
gew
öh
nt.
Un
d m
an
che d
avo
n s
ind
fals
ch u
nd
man
che s
ind
ric
hti
g.
Un
d z
u s
ag
en
, w
o i
st d
a e
igen
tlic
h d
as
Pro
ble
m i
st s
chon
ein
Hin
weis
dara
uf.
Fü
r m
ich
fü
hlt
sic
h d
as
nic
ht
fals
ch a
n e
s zu
sag
en
. Ic
h h
ab
em
ein
e M
od
ell
e w
ie i
ch m
ir v
ors
tell
en
kan
n w
ie d
as
sein
soll
. U
nd
das
war
es.
Kan
nn
atü
rlic
h s
ein
, d
ass
es
da e
in g
ute
s A
rgu
men
t g
ibt,
das
es
nic
ht
so s
ein
soll
te.
Un
dd
an
n m
uss
man
eb
en
wie
der
ein
en
Para
dig
men
wech
sel
irg
en
dw
ie s
chaff
en
.D
esw
eg
en
gla
ub
e i
ch n
ich
t, d
ass
es
ein
e g
run
dle
gen
de Ä
nd
eru
ng
in
dem
Vers
tän
dn
is d
er
Qu
an
ten
mech
an
ik g
eb
en
wir
d.
Eh
er.
.. W
ir s
chärf
en
un
sere
Bil
der
60
.
un
d i
rgen
dw
an
n f
üh
lt s
ich
das
all
es
rech
t ri
chti
g a
n.
Rein
hard
Un
d s
ind
da d
ie E
xperi
men
te s
o e
ine A
rt I
nst
rum
en
t u
m d
en
Um
gan
g b
ess
er
zusc
hu
len
? W
eil
man
hie
r ja
die
Hän
de d
ara
uf
leg
en
kan
n?
61
.
Nik
ola
iB
is z
u e
inem
gew
isse
n G
rad
gla
ub
e i
ch ja.
Ab
er
ich
weiß
nic
ht
ob
es
dara
n l
ieg
t,d
ass
man
Han
d a
nle
gen
kan
n.
Als
o e
in E
xperi
men
t is
t im
mer
die
letz
teE
nts
cheid
un
g.
Man
kan
n s
ich
halt
da n
ich
ts v
orm
ach
en
. U
nd
zw
ar
sch
on
im
Kle
inen
. Ic
h m
ein
e d
as
jetz
t g
ar
nic
ht
nu
r w
en
n m
an
ein
e g
roß
e T
heori
e w
iderl
eg
t,so
nd
ern
sch
on
im
Kle
inen
, w
en
n m
an
ein
fals
ches
Bil
d i
m K
op
f h
at.
Un
d e
s is
t ja
imm
er
wie
der
ers
tau
nli
ch:
Da r
ed
en
wir
mit
jem
an
den
, m
it d
em
man
seit
zw
ei
Jah
ren
arb
eit
et,
un
d p
lötz
lich
bei
der
fun
dam
en
tals
ten
Sach
e m
erk
t m
an
, d
ass
man
eig
en
tlic
h e
in k
om
ple
tt u
nte
rsch
ied
lich
es
Bil
d i
m K
op
f h
at.
Un
d d
an
n w
ett
et
man
meis
ten
s ein
Bie
r d
ara
uf.
Dafü
r, s
chon
im
Kle
inen
die
Bil
der
im K
op
f zu
prä
gen
.
62
.
Rein
hard
Ja,
es
gib
t h
alt
Sic
herh
eit
. D
as
Exp
eri
men
t is
t d
a u
nd
die
s is
t sc
hon
ein
seh
rst
ark
er
Hin
weis
.6
3.
Nik
ola
iIc
h h
ab
e jetz
t le
tzte
s m
al
etw
as
nic
ht
meh
r au
sgere
chn
et,
weil
ich
mir
ged
ach
th
ab
e,
jetz
t lo
hn
t es
sich
nic
ht
meh
r, jetz
t se
hen
wir
es
eh
gle
ich
im
Exp
eri
men
t. E
sw
äre
fals
ch g
ew
ese
n w
as
ich
dach
te d
as
[bei
der
Rech
nu
ng
] ra
usk
om
mt.
In
sofe
rnw
ar
es
die
ric
hti
ge E
nts
cheid
un
g.
Von
dah
er
gla
ub
e i
ch,
dass
die
Exp
eri
men
te a
uf
jed
en
Fall
helf
en
. U
nd
dan
n n
atü
rlic
h,
wie
gesa
gt,
es
gib
t ein
paar
Sach
en
wo m
an
halt
sic
h v
iell
eic
ht
an
Sach
en
gew
öh
nen
kan
n,
die
au
ch n
ich
t ri
chti
g s
ind
. D
iem
uss
man
dan
n a
n e
iner
best
imm
ten
Ste
lle d
an
n w
iderl
eg
en
. D
as
fin
de i
ch g
era
de
das
span
nen
de h
ier
in d
er
Gru
pp
e.
In e
iner
beso
nd
ers
au
sgep
räg
ten
Weis
e h
alt
gesc
hau
t w
ird
wo k
an
n i
ch jetz
t S
ach
en
test
en
, d
ie w
irkli
ch a
n e
ine S
tell
e g
eh
en
,w
o i
ch m
ir w
irkli
ch u
nkla
r b
in w
as
rau
skom
mt.
Wo i
ch n
ich
t sa
ge,
da m
üss
te d
as
jetz
t ra
usk
om
men
, ab
er
sch
au
en
wir
mal
nach
. S
on
dern
wo e
s w
irkli
ch e
infa
chn
ich
t kla
r is
t je
tzt.
Das
ist
span
nn
en
d.
Es
ist
natü
rlic
h d
ie F
rag
e i
n w
elc
hem
Zeit
rah
men
es
pass
iert
, ob
ich
dan
n i
mm
er
noch
das
selb
e m
ach
e?
64
.
En
de
Rein
hard
Von
mein
er
Seit
e a
us
wäre
es
das.
Wen
n d
u n
och
etw
as
sag
en
wil
lst?
65
.(n
o s
peaker)
Gesp
räch
üb
er
den
In
halt
un
d M
oti
vati
on
mein
er
Dip
lom
arb
eit
. U
nd
in
wie
weit
das
Ph
iloso
ph
ie i
st.
Dan
ksa
gu
ng
un
d a
usk
lin
gen
der
small
talk
.6
6.
C Transcription of Interviews
114
Wit
lef_
110510
Inte
rvie
w m
it W
itle
f W
iecz
ore
k v
om
10
.05
.20
11
Tra
nsc
rib
ed
by
yott
a,
vers
ion
4 o
f 1
10
83
0
An
fan
g,
pers
ön
lich
e D
ate
n,
Au
sbil
du
ng
Rein
hard
+ W
itle
f1:
ipod
? W
ie l
an
ge k
an
n m
an
au
fneh
men
?2:
ja,
ext
ern
es
Mik
ro.
So l
an
g B
att
eri
e o
der
Pla
tz r
eic
ht.
1.
1:
Als
o d
u h
ast
es
(DA
-Exp
ose
IV_R
ST.
pd
f) g
ele
sen
? D
.h.
du
weiß
t u
ng
efä
hr
um
was
es
geh
t. D
ie F
rag
en
werd
en
, d
an
n e
h n
ich
t so
sp
ezi
ell
sein
.2:
Ja,
ich
hab
es
gele
sen
.
2.
Rein
hard
Am
An
fan
g w
ill
ich
eig
en
tlic
h n
ur
seh
r g
en
ere
lle S
ach
en
wis
sen
. Z
.B.
dein
Alt
er?
3.
Wit
lef
32
. Post
-Doc.
Seit
ein
em
Jah
r h
ier.
Davo
r in
Mü
nch
en
gew
ese
n.
Da w
ar
ich
vie
rJa
hre
Dokto
ran
d.
Mu
ltip
hoto
nen
vers
chrä
nku
ng
gem
ach
t. U
nd
davo
r d
ieD
iplo
marb
eit
in
Berl
in.
Da h
ab
e i
ch g
ar
nic
ht
Vers
chrä
nku
ng
gem
ach
t, d
a w
are
nes
eh
er
Qu
an
ten
pu
nkte
.
4.
Rein
hard
D.h
. ab
er
son
st b
ist
du
eig
en
tlic
h z
iem
lich
in
dem
Feld
jetz
t d
rin
nen
?5
.W
itle
fJa
, sc
hon
wir
kli
ch jetz
t lä
ng
ere
Zeit
. S
o f
ün
f, s
ech
s Ja
hre
.6
.
Moti
vati
on
Rein
hard
Grü
nd
e w
aru
m d
u d
as
mach
st?
Fall
s m
an
sow
as
üb
erh
au
pt
an
geb
en
kan
n.
7.
Wit
lef
Als
o g
en
au
jetz
t O
pto
mech
an
ik o
der
an
sic
h P
hys
ik,
Qu
an
ten
info
rmati
on
,...
?8
.R
ein
hard
Fan
gen
wir
mit
dem
All
gem
ein
sten
an
, P
hys
ik ü
berh
au
pt?
Waru
m t
ut
man
sic
h d
as
an
?9
.
Wit
lef
Ich
bin
ein
bis
sch
en
vorg
ep
räg
t d
urc
h m
ein
en
Vate
r w
ah
rsch
ein
lich
, w
eil
der
ist
selb
st P
hys
iker.
Un
d h
at
au
ch a
ls P
hys
iker
gearb
eit
et,
au
ch a
ls E
xperi
men
tato
r.A
ber
ein
fach
nu
r vo
n z
uh
au
se.
Da w
are
n i
rgen
d w
ie i
mm
er
nu
r ir
gen
dw
elc
he
Gerä
te z
uh
au
se.
Irg
en
dw
as
zum
löte
n u
nd
so ;
un
d h
ab
das
halt
gem
ach
t.
10
.
Ab
er
als
an
gefa
ng
en
hab
zu
stu
die
ren
wu
ßte
ich
gar
nic
ht,
dass
ich
Ph
ysik
mach
en
woll
te.
Als
o i
ch w
oll
te s
chon
was
natu
rwis
sen
sch
aft
lich
es
mach
en
, w
eil
das
au
chin
der
Sch
ule
tota
l vi
el
Sp
aß
gem
ach
t h
at.
In
der
Sch
ule
wars
gar
nic
ht
mal
eig
en
tlic
h P
hys
ik w
as
rich
tig
, ri
chti
g v
iel
Sp
aß
gem
ach
t h
at.
Da w
ar
es
eh
er
Ch
em
ie,
ab
er
das
lag
ein
bis
sch
en
am
Leh
rer.
Dan
n w
oll
te s
o e
in K
reu
zfach
stu
die
ren
, so
wie
Bio
ph
ysik
od
er
ph
ysik
ali
sch
e C
hem
ie.
Ab
er
das
gab
es
nic
ht
sori
chti
g i
n B
erl
in.
Ich
hab
au
ch n
ich
t w
eit
er
geku
ckt.
Ich
weiß
au
ch n
ich
t m
eh
rw
aru
m.
Jetz
t w
ürd
e i
ch e
s m
ach
en
, ab
er
dam
als
halt
nic
ht.
11
.
Un
d d
an
n h
ab
e i
ch h
alt
Ph
ysik
stu
die
rt,
weil
irg
en
dw
ie h
ab
en
mic
h E
xperi
men
ted
ah
in g
eb
rach
t. W
eil
dort
an
der
TU
Berl
in g
ab
s so
was
wie
ein
Pra
kti
ku
m,
Pro
jektl
ab
or
hie
ß d
as,
wo m
an
halt
in
der
Gru
pp
e g
leic
h z
usa
mm
en
an
fän
gt
zu
12
.
arb
eit
en
un
d n
ich
t sc
hon
die
Exp
eri
men
te a
ufg
eb
au
t si
nd
. M
an
mu
sste
sic
h h
alt
selb
st e
ins
üb
erl
eg
en
, p
lan
en
, au
fbau
en
un
d a
usw
ert
en
. A
lso d
as
war
tota
l g
en
ial.
Un
d Q
uan
ten
info
rmati
on
? D
ah
in b
in i
ch e
igen
tlic
h e
rst,
als
o b
in i
ch w
äh
ren
d d
es
Stu
diu
ms
gekom
men
, w
eil
ich
au
ch o
f so
ein
er
Som
mers
chu
le w
ar,
die
halt
üb
er
Qu
an
ten
info
rmati
on
war.
Un
d d
a w
ar
der
Rein
hard
Wern
er
un
d d
er
Jen
s E
isert
,u
nd
ich
gla
ub
e d
ie s
ind
ein
bis
sch
en
bekan
nt.
Beid
es
Th
eore
tiker
un
d g
era
de d
er
Rein
hard
Wern
er
kon
nte
mic
h t
ota
l d
afü
r b
eg
eis
tern
. D
en
n e
r h
at
au
ch s
ozu
sag
en
gesa
gt,
ja d
a g
ibts
halt
Pro
ble
me m
it B
ell
'sch
er
Un
gle
ich
un
g.
Un
d i
rgen
dw
iese
itd
em
hat
mic
h d
as
eig
en
tlic
h i
nte
ress
iert
.
13
.
Rein
hard
Als
o d
as
fän
gt
eig
en
tlic
h s
chon
an
mit
der
Pro
ble
mst
ell
un
g s
ozu
sag
en
. A
lso w
en
nd
u d
a s
ag
st,
dass
du
gen
au
dort
...,
au
fzu
zeig
en
, d
er
ers
te K
on
takt,
un
d d
as
es
eb
en
nic
ht
so e
infa
ch i
st.
14
.
Wit
lef
Ja,
das
war
au
ch s
o e
in b
issc
hen
der
Vort
rag
wie
er
ihn
gem
ach
t h
at.
Er
[Rein
hard
Wern
er]
ist
ein
Men
sch
der
den
Lap
top
nic
ht
nu
r als
Beam
erp
roje
kto
r n
imm
t,so
nd
ern
au
ch d
en
Sou
nd
. E
r h
at
halt
so D
ete
kto
ren
geh
ab
t, d
ie d
an
n s
o g
ekli
ckt
hab
en
[E
PR
/BE
LL
Exp
eri
men
t].
Un
d d
an
n h
at
er
au
ch g
esa
gt
das
Ein
stein
das
Pap
er
[EP
R A
rtik
el]
rau
sgeb
rach
t h
at.
Un
d e
s p
ass
iert
ja n
ich
t so
oft
: A
) D
ass
es
nic
ht
so z
itie
rt w
ird
, g
leic
h a
m A
nfa
ng
; a
lso e
s w
urd
e ja g
ar
nic
ht
ziti
ert
am
An
fan
g.
Un
d,
dass
ers
t d
reiß
ig J
ah
r g
ed
au
ert
hat
bis
dan
n e
ine A
ntw
ort
kam
. D
as
man
es
exp
eri
men
tell
mess
en
kan
n.
Un
d d
as
war
dan
n i
rgen
dw
ie s
pan
nen
d.
Die
Gesc
hic
hte
halt
war
span
nen
d,
un
d d
an
n d
as
Pro
ble
m h
alt
au
ch.
15
.
Au
sbil
du
ng
Rein
hard
Fast
ein
kla
ssic
her
Ein
stie
g,
ich
wü
sste
jetz
t n
ich
t w
ie d
ies
so..
.1
6.
Wit
lef
Weil
im
Stu
diu
m w
ar
das
gar
nic
ht,
als
o k
am
das
gar
nic
ht
vor
bei
un
s.1
7.
Rein
hard
Im S
tud
ium
selb
st n
ich
t?1
8.
Wit
lef
Ja d
as
hän
gt
von
der
Un
ivers
ität
ab
.1
9.
Rein
hard
Wie
war
da d
er
Zu
gan
g f
ür
jetz
t Q
uan
ten
mech
an
ik?
Rein
nu
r...
20
.W
itle
fK
ast
en
pote
nti
al,
Wass
ers
toff
ato
m,
dan
n S
töru
ng
srech
nu
ng
, D
iracf
orm
ali
smu
s.A
ber
nie
irg
en
dw
ie d
iese
s P
rob
lem
an
gesp
roch
en
. A
ber
das
hän
gt
von
der
Un
i ab
.2
1.
Rein
hard
Ab
er
wie
hab
en
die
das
dan
n e
xperi
men
tell
verb
un
den
, od
er
hat
es
das
dan
n n
ich
tg
eg
eb
en
?2
2.
Wit
lef
Sozu
sag
en
in
der
Un
i, i
n d
en
Vorl
esu
ng
en
? N
e g
ar
nic
ht.
Als
o h
alt
die
hab
en
nie
erw
äh
nt
das
es
Bell
'sch
e U
ng
leic
hu
ng
en
gib
t. O
der
das
es
Exp
eri
men
te d
azu
gib
t.O
der
das
es
halt
ein
Pro
ble
m g
ibt.
Un
d b
ei
der
Inte
rpre
tati
on
nu
ll.
23
.
Ab
er
ich
gla
ub
e d
as
hän
gt
halt
wir
kli
ch d
avo
n a
b w
o d
ie a
uch
selb
st g
ele
rnt
hab
en
. U
nd
ob
sie
es
halt
rein
bri
ng
en
woll
en
. Ic
h m
ein
man
hätt
e e
s au
ch b
ei
stati
stis
cher
Ph
ysik
mach
en
kön
nen
, d
a w
är
es
au
ch g
eg
an
gen
. Ir
gen
dw
o,
Dic
hte
matr
ix,
Qu
an
ten
form
ali
smu
s h
ätt
e m
an
es
ein
fach
mach
en
kön
nen
, h
ab
en
sie a
ber
nic
ht.
24
.
Rein
hard
115
D.h
. es
ist
fast
rein
beim
Form
ali
smu
s g
eb
lieb
en
un
d..
.2
5.
Wit
lef
Gen
au
, es
ist
ein
fach
Form
ali
smu
s oh
ne I
nte
rpre
tati
on
. O
der
oh
ne F
olg
en
.2
6.
Rein
hard
Oh
ne g
roß
moti
viert
[zu
werd
en
]. E
s g
eh
t zw
ar
üb
er
Wass
ers
toff
, d
as
Kast
en
pote
nti
al,
usw
. A
ber
es
nic
ht
so..
.2
7.
Au
fgab
e i
m E
xp
eri
men
t
Rein
hard
Ja,
jetz
t b
ist
du
da i
n d
er
Gru
pp
e u
nd
hast
das
Exp
eri
men
t ü
ber.
28
.W
itle
fÜ
ber?
Als
o d
as
ich
es
nic
ht
meh
r m
ag
?2
9.
Rein
hard
Nein
, als
o d
ass
du
der
Hau
ptz
ust
än
dig
e b
ist.
30
.W
itle
fA
h !
Zu
r Z
eit
ja.
Als
o w
eil
der
Sim
on
[G
röb
lach
er]
. S
imon
hat
ja p
rakti
sch
an
dem
Exp
eri
men
t se
ine D
okto
rarb
eit
dra
n g
esc
hri
eb
en
. E
r h
at
das
au
fgeb
au
cht.
Un
d e
ris
t je
tzt
halt
als
Post
-Doc
am
CalT
ech
[C
ali
forn
ia I
nst
itu
te o
f Tech
nolo
gy]
. Teil
weis
ed
ort
, te
ilw
eis
e h
ier.
Un
d i
ch m
an
ag
e p
rakti
sch
das
Exp
eri
men
t ;
bau
e d
a a
uf.
Un
dw
ir s
ind
ja g
era
de a
m U
mzi
eh
en
. "Ü
ber"
ist
lu
stig
. B
ei
un
s w
ürd
e d
as
heiß
en
, d
ass
du
es
nic
ht
meh
r m
ag
st.
Hast
du
das
Exp
eri
men
t je
tzt
sch
on
üb
er!
?
31
.
Ne,
als
o v
on
dah
er
bin
jetz
t p
rakti
sch
Hau
ptv
era
ntw
ort
lich
er.
Ab
er
zur
Zeit
ste
ht
ich
halt
pra
kti
sch
nu
r im
Lab
or.
32
.
Rein
hard
Ja i
st k
lar,
jetz
t m
it d
em
Um
zug
.3
3.
Wit
lef
Ich
besc
häft
ige m
ich
im
Mom
en
t n
ich
t so
vie
l m
it T
heori
e.
Das
ist
ein
bis
sch
en
Sch
ad
e,
weil
ich
fin
de g
era
de a
ls P
ost
-Doc
wäre
das
gera
de e
ine A
ufg
ab
e u
nd
sic
hau
ch ü
berl
eg
en
was
man
fü
r zu
kü
nft
ige E
xperi
men
te m
ach
en
kan
n.
Un
d w
eil
es
halt
wic
hti
g i
st,
in d
em
Feld
an
sich
, w
elc
he F
rag
est
ell
un
gen
man
bean
twort
en
wil
l.A
ber
dafü
r h
ab
e i
ch g
ar
kein
e Z
eit
.
34
.
Rein
hard
Als
o d
as
wäre
der
zukü
nft
ige A
bla
uf
?3
5.
Wit
lef
Ja h
off
e i
ch m
al
!3
6.
Rein
hard
Als
o s
o s
tell
t d
u e
s d
ir v
or.
Als
o s
o h
ätt
est
du
es
gern
e.
Wen
n d
er
Um
zug
ab
gesc
hlo
ssen
ist
, d
ass
du
dan
n a
uch
arb
eit
stech
nis
ch z
ukü
nft
ige S
ach
en
,exp
eri
men
tell
e..
. ab
er
au
f d
er
Basi
s vo
n d
em
vorh
an
den
en
.
37
.
Wit
lef
Un
sere
Basi
s zu
r Z
eit
ist
, re
in e
xperi
men
tell
, u
nse
r D
elu
tion
Fri
dg
e.
Wir
hab
en
halt
die
Mög
lich
keit
au
f ti
efe
Tem
pera
ture
n z
u g
eh
en
un
d d
am
it m
ech
an
isch
eS
yste
me e
ntw
ed
er
dir
ekt
in d
en
Gru
nd
zust
an
d z
u k
üh
len
. A
lso w
en
n s
ie h
alt
ein
eh
oh
e F
req
uen
z g
leic
h v
on
sic
h a
us
hab
en
. O
der
halt
zu
sätz
lich
, h
ab
en
wir
ein
en
ied
rig
e B
ad
tem
pera
tur,
un
d d
an
n z
usä
tzli
ch d
as
Seit
en
ban
d k
üh
len
um
in
den
Gru
nd
zust
an
d z
u g
eh
en
. D
.h.
das
ist
un
sere
Mög
lich
keit
die
wir
hab
en
un
d jetz
t,sa
gen
wir
so,
wart
en
wir
ein
fach
au
f d
ie r
ich
tig
en
Pro
ben
, S
am
ple
s, d
ie e
ntw
ed
er
das
ein
e m
ach
en
od
er
das
an
dere
, od
er
beid
es.
Un
d d
an
n g
eh
ts v
on
den
Exp
eri
men
ten
au
sgeh
en
d w
eit
er.
38
.
Rein
hard
Als
o,
dass
man
das
so a
ls B
asi
s od
er
Au
sgan
gse
xperi
men
t h
at
un
d d
an
n s
chli
eß
en
39
.
sich
...
Wit
lef
Gen
au
, u
nd
dan
n s
chli
eß
en
sic
h d
ie S
ach
en
die
wir
eig
en
tlic
h m
ach
en
woll
en
an
.4
0.
Rein
hard
Es
ist
ja s
o u
nd
so n
ie e
in E
xperi
men
t, d
ass
du
au
fbau
st u
nd
dan
n e
in E
rgb
nis
hast
un
d d
an
n w
ied
er
ab
reis
st.
41
.
Wit
lef
Pass
iert
au
ch,
ab
er
bei
un
s h
alt
nic
ht.
42
.
Ein
teil
un
g d
er
Exp
eri
men
te
Rein
hard
Ein
e n
äch
ste F
rag
e w
äre
dan
n w
ie d
ie G
rup
pe a
ufg
eb
au
t is
t? W
en
n d
u jetz
t, w
ieim
mer
man
das
nen
nt,
Hau
ptv
era
ntw
ort
lich
er
bis
t b
ei
dem
Exp
eri
men
t ;
den
n e
sg
ibt
ja m
eh
rere
para
llel.
Es
sin
d ja n
och
die
gep
uls
ten
Sach
en
...
43
.
Wit
lef
Fan
gen
von
den
Nan
ote
ilch
en
, u
nd
noch
Str
ah
lun
gsd
ruck
gan
z ein
fach
gib
ts n
och
,u
nd
der
Jon
as
[Sch
möle
] h
att
e,
ab
er
der
mach
t je
tzt
sozu
sag
en
bei
un
s m
it.
Er
hatt
e d
avo
r h
alt
mag
neti
sch
levi
tiert
e S
ach
en
; G
rap
hit
un
d s
ow
as.
44
.
Rein
hard
Das
sin
d a
lso d
ie T
eil
e d
ie p
ara
llel
lau
fen
?4
5.
Wit
lef
Gen
au
, als
o p
rakti
sch
das
gro
ße T
hem
a i
n d
er
Arb
eit
gru
pp
e,
an
sic
h d
er
Au
fhän
ger,
wofü
r si
ch h
alt
Mark
us
[Asp
elm
eye
r] i
nte
ress
iert
un
d d
am
it w
ir a
uch
,si
nd
ein
fach
makro
skop
isch
e S
yste
me.
Sys
tem
e a
lso d
ie M
ass
e h
ab
en
in
Qu
an
ten
zust
än
de z
u b
rin
gen
. U
nd
da g
ibts
jetz
t ve
rsch
ied
en
eH
era
ng
eh
en
sweis
en
. E
ntw
ed
er
so w
ie w
ir.
Wir
kü
hle
n h
alt
irg
en
dw
elc
he
Osz
illa
tore
n.
Hat
den
Nach
teil
, d
ie h
ab
en
halt
im
mer
irg
en
dw
ie e
ine V
erb
ind
un
gzu
r A
uß
en
welt
.
46
.
Rein
hard
Ja,
du
mu
sst
sch
au
en
, d
ass
du
die
Um
welt
ein
flü
sse s
ozu
sag
en
weg
kri
eg
st.
Tem
pera
tur
in d
em
Sin
n ?
47
.
Wit
lef
Tem
pera
tur,
gen
au
. O
der
Verb
ind
un
gen
. D
as
An
dere
was
halt
Nik
ola
i [K
iese
l]m
ach
t m
it d
iese
n N
an
ote
ilch
en
, d
ie h
ab
en
halt
gar
kein
e V
erb
ind
un
g m
eh
r zu
rU
mw
elt
. D
ie s
ind
halt
nu
r li
mit
iert
du
rch
Dru
ck v
on
au
ßen
, od
er
Ab
sorb
tion
. U
nd
der
Jon
as
[Sch
möle
] h
at
halt
was
an
dere
s ve
rsu
cht,
mag
neti
sch
zu
levi
tiere
n.
Das
sin
d e
infa
ch v
ers
chie
den
e H
era
ng
eh
en
sweis
en
um
irg
en
dw
ie s
o Q
uan
ten
zust
än
de
bei
die
sen
Sys
tem
en
hin
zub
ekom
men
.
48
.
Un
d s
ag
en
wir
mal
die
Str
uktu
r vo
n u
nse
rer
Gru
pp
e i
st e
igen
tlic
h,
rela
tive
lose
. In
dem
Sin
ne, d
ass
es
jetz
t n
ich
t ein
gig
an
tisc
hes
Pro
jekt
gib
t, w
ora
n a
lle d
ara
narb
eit
en
. S
on
dern
es
gib
t h
alt
die
se v
ers
chie
den
en
...
49
.
Rein
hard
Das
Pri
nzi
p,
od
er
das
Kon
zep
t d
ah
inte
r is
t eb
en
die
se o
pto
-mech
an
isch
e..
.Verk
op
plu
ng
.5
0.
Wit
lef
Gen
au
. A
ber
um
eh
rlic
h z
u s
ein
ich
gla
ub
e w
en
n m
an
jetz
t n
ur
an
makro
skop
isch
en
Qu
an
ten
zust
än
den
in
tere
ssie
rt i
st o
der
irg
en
dw
ie m
ass
ive
Ob
jekte
dah
in z
u b
rin
gen
, d
an
n i
st e
s eig
en
tlic
h e
gal
was
man
neh
men
wü
rde.
Ab
er
sozu
sag
en
die
Op
tom
ech
an
ik i
st h
alt
gera
de s
o w
eit
, d
ass
sie
ku
rz d
avo
r is
td
as
zu e
rreic
hen
.
51
.
Rein
hard
C Transcription of Interviews
116
Das
ist
ja d
as
Sch
ön
e,
dass
die
Reali
sieru
ng
von
Qu
an
ten
zust
än
den
zie
mli
ch o
ffen
ist.
Als
o e
s is
t ja
nic
ht
ein
e B
ind
un
g a
n i
rgen
dein
Sys
tem
, so
nd
ern
es
sin
dte
chn
isch
e F
rag
en
. W
en
n i
ch m
it d
er
Min
itu
tris
ieru
ng
im
Mech
an
isch
en
, w
eil
ich
das
halb
weg
s im
Gri
ff h
ab
e,
die
meach
an
isch
en
Kom
pon
en
ten
hin
zukri
eg
en
. W
en
nd
as
halt
so f
un
kti
on
iert
kan
n m
an
das
dam
it A
nst
reb
en
.
52
.
In d
em
Sin
n g
ibt
es
ja k
ein
e A
bh
än
gig
keit
von
der
Reali
sieru
ng
. A
lso w
ie i
ch d
iese
Sach
en
vers
uch
e z
u r
eali
sere
n.
53
.
Gru
pp
e
Wit
lef
Wir
sin
d h
alt
rela
tiv
Post
-Doc
last
ig.
Un
sere
Arb
eit
sgru
pp
e i
st jetz
t n
ich
t so
typ
isch
. Ic
h w
ürd
e s
chon
eh
er
sag
en
, d
ass
es
meis
ten
s so
ist
: E
s g
ibt
ein
paar
Post
-Docs
, d
ie jew
eil
s fü
r so
ein
Exp
eri
men
t ve
ran
twort
lich
sin
d.
Un
d d
an
n g
ibts
zwei
bis
dre
i D
okto
ran
den
pro
Exp
eri
men
t. U
nd
bei
un
s is
t es
halt
nic
ht
so.
Wir
hab
en
meh
r Post
-Docs
, od
er
gen
au
sovi
el
Post
-Docs
wie
Dokto
ran
den
od
er
kn
ap
pw
en
iger
Dokto
ran
den
un
d w
en
ig M
ast
ers
tud
en
ten
. A
lso s
chon
nic
ht
so t
ypis
ch.
Ab
er
das
kom
mt
viell
eic
ht
au
ch e
infa
ch d
ah
er
das
Mark
us
[Asp
elm
eye
r] e
ben
noch
nic
ht
sola
ng
e h
ier
ist.
Un
d d
as
es
sich
hie
r ers
t ru
msp
rech
en
mu
ss,
dass
es
die
Exp
eri
men
te g
ibt
un
d d
en
Nach
wu
chs
an
zule
rnen
.
54
.
Rein
hard
Ja d
as
dau
ert
bis
du
die
Leu
te r
ein
kri
eg
st.
Weil
beg
inn
en
wir
st d
u s
o u
nd
so m
iterf
ah
ren
ere
n L
eu
ten
. A
lso f
än
gst
du
mit
Post
-Docs
an
, d
am
it d
as
ein
mal
läu
ft.
Üb
erh
au
pt
wen
n e
s n
eu
ist
, d
an
n w
irst
du
dir
nic
ht
noch
am
An
fan
gE
inarb
eit
un
gsz
eit
[au
fhals
en
].
55
.
Fasz
inati
on
an
der
Qu
an
tem
mech
an
ik
Rein
hard
Ein
e F
rag
e i
m t
heore
tisc
hen
Bere
ich
. O
der
wir
hab
en
darü
ber
eh
sch
on
mal
gesp
roch
en
.Was
wü
rdest
du
als
fasz
inie
ren
stes
Featu
re s
eh
en
, vo
n d
er
Qu
an
ten
mech
an
ik.
Eig
en
tlic
h b
is d
u ja e
h i
n d
em
Bere
ich
der
dic
h i
nte
ress
iert
.
56
.
Wit
lef
Zu
r Z
eit
ja.
Wech
selt
. A
lso i
ch fi
nd
e s
eh
r sp
an
nen
d w
irkli
ch w
as
wir
mach
en
, als
od
as
Zie
l vo
n u
ns.
Das
man
wir
kli
ch v
ers
uch
t m
it S
yste
men
, d
ie h
alt
vie
l M
ass
eh
ab
en
, als
o i
m V
erg
leic
h h
alt
zu
Ato
men
, Io
nen
, od
er
Ato
mw
olk
en
,Q
uan
ten
zust
än
de z
u e
rzeu
gen
. U
nd
dan
n h
alt
au
ch a
m I
deals
ten
natü
rlic
h z
wei
mass
ive S
ach
en
mit
ein
an
der
zu v
ers
chrä
nken
. F
ind
e i
ch s
chon
tota
l sp
an
nen
d.
Un
d i
mm
er
meh
r kom
mt
dazu
, ab
er
da k
en
ne i
ch m
ich
leid
er
noch
zu
wen
ig a
us,
inw
iew
eit
Gra
vita
tion
ein
e R
oll
e s
pie
lt.
Als
o d
ie v
ers
chie
den
en
Dekoh
äre
nzm
od
ell
e.
Ken
ne i
ch m
ich
leid
er
zuw
en
ig a
us,
ab
er
es
wir
d e
in S
em
inar
geb
en
. U
nd
da b
in i
ch z
iem
lich
fro
h d
rüb
er,
dass
wir
das
mach
en
. D
en
n i
stn
och
ein
mal
ein
gan
z an
dere
r A
spekt
mit
dem
ich
halt
nie
in
Berü
hru
ng
gekom
men
bin
.
57
.
Vers
chrä
nku
ng
an
sic
h i
st a
uch
sp
an
nen
d.
Als
o,
man
kan
n s
ich
halt
im
mer
wie
der
Fra
gen
, w
ie i
nte
rpre
tiert
man
die
s n
un
; m
it u
nse
rer
kla
ssic
hen
Welt
.Ich
fin
de n
ur
ein
bis
sch
en
wir
d e
s zu
vie
l b
eto
nt.
Ich
fan
d e
s ein
bis
sch
en
so w
ie d
u e
sg
esc
hri
eb
en
hast
in
dein
er
Ein
leit
un
g,
dass
man
vie
lleic
ht
ein
bis
sch
en
üb
ers
trap
azi
ert
um
halt
irg
en
dw
ie d
as
Beso
nd
ere
im
mer
wie
der
hera
usz
ukeh
ren
58
.
Rein
hard
Das
ist
eb
en
die
Fra
ge o
b m
an
das
jetz
t n
ur.
..5
9.
Wit
lef
Ist
An
sich
tssa
che,
ist
ein
pers
ön
lich
er
Gesc
hm
ack
. Je
der
wü
rde d
a s
ich
er
etw
as
an
dere
s sa
gen
, ab
er
nic
hts
dest
otr
otz
ist
es
halt
wir
kli
ch e
ine P
rob
lem
. W
eil
man
halt
best
imm
te A
nn
ah
men
mach
t w
ie L
okali
tät,
Reali
smu
s u
nd
das
Qu
an
ten
mech
an
ik e
ine k
om
ple
tte T
heori
e i
st,
dan
n s
ieh
t m
an
zu
r Z
eit
ist
es
ein
fach
nic
ht
so u
nd
dan
n h
at
man
wir
kli
ch e
in P
rob
lem
. W
as
ich
halt
ein
bis
sch
en
Sch
ad
e fi
nd
e,
dass
es
vers
chie
den
e M
ein
un
gen
gib
t, d
as
ist
ja o
k,
gib
ts ja i
mm
er,
ab
er,
dass
dan
n m
it d
en
Leu
ten
nic
ht
meh
r d
isku
tiere
n k
an
n.
Es
gib
t h
alt
so
Sch
ule
n,
die
sin
d h
alt
so,
die
an
dere
n s
o u
nd
das
wars
. E
ine D
isku
ssio
n k
an
n m
an
dan
n v
erg
ess
en
. D
as
ist
halt
Sch
ad
e,
dan
n w
ird
halt
etw
as
au
fged
rück
t, i
st m
an
pass
iver
Zu
höre
r u
nd
es
ist
die
Fra
ge o
b m
an
da w
as
lern
t.
60
.
Rein
hard
Ja,
die
Fra
ge i
st v
on
wo s
ozu
sag
en
die
In
terp
reta
tion
herk
om
men
. F
ür
mic
hsc
hein
t es
von
der
Th
eori
e h
er
zu k
om
men
; d
ie s
teh
en
am
Sch
eid
ew
eg
. D
ie F
rag
eis
t w
ie d
ies
exp
eri
men
tell
rele
van
t is
t. W
en
n m
an
es
gan
z ru
nte
rbri
cht
au
f g
an
zein
fach
e A
rbeit
en
im
Lab
or
ist
ja d
as
all
es
irre
leva
nt.
61
.
Wit
lef
Völl
ig k
lar.
Da i
st e
s ers
tmal
Wu
rst.
Es
ist
halt
In
spir
ati
on
.6
2.
Rein
hard
Ja,
Ja.
Es
geh
t d
an
n e
her
in R
ich
tun
g d
er
Sach
en
, d
ie d
as
Exp
eri
men
t m
oti
viere
n.
Waru
m w
ill
ich
eig
en
tlic
h e
ine V
ers
chrä
nku
ng
mit
mass
ivere
n T
eil
en
?6
3.
Wit
lef
Ich
gla
ub
e d
as
ist
eb
en
, fi
nd
e i
ch,
zum
ers
ten
mal
wir
kli
ch f
ür
mic
h a
uch
ein
eri
chti
ge M
oti
vati
on
an
Vers
chrä
nku
ng
weit
erz
uarb
eit
en
, w
eil
man
sic
h h
alt
wir
kli
ch e
ine k
on
kre
te F
rag
est
ell
un
g s
tell
en
kan
n,
in d
em
Sin
ne,
welc
he R
oll
esp
ielt
Gra
vita
tion
. A
lso g
eh
ts b
ei
mass
iven
Ob
jekte
n o
der
kan
n m
an
wir
kli
ch s
oD
ekoh
äre
nzm
od
ell
e s
eh
en
. U
nd
das
fin
de i
ch w
ied
er
gu
t, w
eil
es
hat
für
mic
h w
as
kon
kre
tere
s als
zu
sag
en
....
Ich
mein
e,
dass
weiß
ich
jetz
t sc
hon
, d
ass
ist
halt
wie
mit
Lokali
tät
- R
eali
smu
s, d
as
geh
t h
alt
nic
h z
usa
mm
en
. A
ber
da g
ibts
halt
zu
r Z
eit
kein
e A
ntw
ort
dra
uf.
Da k
an
n m
an
die
Bell
Un
gle
ich
un
g z
eh
nta
use
nd
mal
verl
etz
en
. D
ie w
urd
e e
infa
ch v
erl
etz
t, d
as
reic
ht.
64
.
Rein
hard
Es
sch
ein
t so
, m
uss
t d
u s
ag
en
ob
du
au
ch s
o d
en
kst
, d
ass
du
von
der
Seit
e [
hie
r is
tT
heori
e g
em
ein
t] k
au
m e
ine A
ntw
ort
od
er
Neu
es
erw
art
en
kan
nst
. D
ie B
ell
Un
gle
ich
un
gen
sin
d t
heore
tisc
h a
ufg
est
ell
t, d
ie E
xperi
men
te d
azu
gib
ts u
nd
man
wir
d n
och
seh
r vi
ele
mach
en
kön
nen
, ab
er
im E
nd
eff
ekt.
..
65
.
Wit
lef
Man
bra
uch
t h
alt
irg
en
dw
ie e
ine n
eu
e T
heori
e,
die
ein
em
das
halt
erk
lärt
od
er
man
test
et
mal
in e
ine a
nd
ere
Ric
htu
ng
.6
6.
Rein
hard
Ab
er
selb
st s
o e
twas
wie
ein
e n
eu
e T
heori
e w
urd
e a
uch
wie
der
etw
as
exp
eri
mete
lles
viell
eic
ht
nach
sich
zieh
en
. S
o w
äre
es
so w
ie d
u s
chon
gesa
gt
hast
neb
en
bei
wie
der
ein
e n
eu
e M
ein
un
g o
der
Inte
rpre
tati
on
.
67
.
Wit
lef
Ich
mein
e e
s g
ibt
halt
vie
le V
erf
ein
eru
ng
en
zu
r B
ell
'sch
en
Un
gle
ich
un
g.
Eb
en
das
Leg
gett
-Mod
ell
[N
ob
elp
reis
träg
er
Sir
An
thon
y Ja
mes
Leg
gett
], d
ass
er
halt
an
nim
mt,
ein
en
Teil
Nic
ht-
Lokali
tät
rein
bri
ng
t, d
ass
das
wie
der
au
sgesc
hlo
ssen
werd
en
kan
n.
Das
ist
halt
fü
r m
ich
nu
r ein
kle
iner
neu
er
Asp
ekt.
Das
löst
fü
r m
ich
au
ch n
ich
t d
as
Pro
ble
m.
Od
er
das
man
halt
fra
gt
wie
viel
Lokali
tät
mu
ss s
o e
ine
Th
eori
e h
ab
en
un
d d
as
kan
n m
an
halt
fast
au
f N
ull
red
uzi
ere
n.
Ja,
ab
er
man
fra
gt
sich
wie
sch
nell
die
se I
nfo
rmati
on
hin
un
d h
er
flie
gt,
mit
wie
viel
Mal
Üb
erl
ich
tgesc
hw
ind
igkeit
. A
ber
mir
pers
ön
lich
gib
t d
ies
kein
e A
ntw
ort
. Is
t ab
er
halt
au
ch G
esc
hm
ack
ssach
e.
68
.
Rein
hard
117
Ja,
ab
er
imm
erh
in g
ibt
es
Grü
nd
e w
aru
m m
an
exp
eri
men
tell
vera
nla
gt
ist
od
er
waru
m m
an
in
exp
eri
men
tell
e S
ach
en
geh
t. D
a s
ieh
t m
an
halt
ein
en
Meh
rwert
im
Exp
eri
men
t. E
s g
ibt
ja e
inen
Gru
nd
waru
m m
an
als
Exp
eri
men
tato
r n
ich
tT
heore
tiker
gew
ord
en
ist
, w
eil
...
69
.
Wit
lef
Ab
er
ich
hab
e m
ich
das
noch
nie
gefr
ag
t u
m e
hrl
ich
zu
sein
. A
lso e
s m
ach
t sc
hon
Sp
ass
im
Lab
or
zu s
ein
un
d r
um
zusc
hra
ub
en
. U
nd
halt
sozu
sag
en
die
theore
tisc
hen
Sach
en
wir
kli
ch u
mzu
setz
en
, u
nd
da k
om
men
dan
n n
och
mal
an
dere
Fra
gen
au
f. W
en
n m
an
sow
as
wie
ein
e F
rom
el
hin
gesc
hri
eb
en
hat,
ein
e G
leic
hu
ng
od
er
hie
r w
ie e
ine P
uls
seq
uen
z, w
ie i
mp
lem
en
tiere
ich
das?
Ja,
ich
kan
n m
ir a
ber
au
ch v
ors
tell
en
sch
on
th
eore
tisc
h z
u A
rbeit
en
. Ic
h w
eiß
nic
ht
inw
iew
eit
ich
das
Lab
or
verm
isse
n w
ürd
e.
Ich
wü
rde e
s sc
hon
verm
isse
n, ab
er
ob
es
sow
eit
geh
t,d
ass
ich
nic
ht
theore
tisc
h a
rbeit
en
kön
nte
? Ic
h h
ab
e h
alt
ein
fach
nic
ht
die
Au
sbil
du
ng
.
70
.
Rein
hard
Ich
tu
e m
ich
im
mer
sch
wer
mit
die
ser
Tre
nn
un
g,
weil
fü
r d
ie g
an
zen
Exp
eri
men
teb
rau
chts
du
so u
nd
so e
inen
zie
mli
chen
Teil
von
Th
eori
e.
Die
gan
zen
kon
tin
uie
rlic
hen
Vari
bale
n V
ers
chrä
nku
ng
[th
eore
tisc
he V
ora
uss
etz
un
g f
ür
das
ind
er
Dip
lom
arb
eit
beh
an
delt
e o
pto
-mech
. E
xperi
men
t] u
nd
so w
eit
er.
Es
ist
ja n
ich
tso
leic
ht,
den
n e
s is
t ein
zie
mli
cher
Blo
ck d
er
vora
us[
gese
tzt
ist]
.
71
.
Wit
lef
Od
er
den
Ham
ilto
nia
n u
m d
en
Osz
illa
tor
zu b
esc
hre
iben
, D
ekoh
äre
nzm
od
ell
e u
nd
so w
eit
er.
Das
ist
all
es
Th
eori
e.
72
.
Rein
hard
Es
ist
ja n
ich
t so
, d
ass
es
vora
uss
etz
un
glo
s w
äre
. A
lso,
dass
du
nu
r in
s L
ab
or
geh
stu
nd
da h
eru
md
reh
st.
Ab
er
das
ist
für
mic
h d
as
Inte
ress
an
te,
inw
iew
eit
die
Fra
gen
üb
erh
au
pt
dan
n n
och
rele
van
t si
nd
.
73
.
Wit
lef
Als
o,
wen
n i
ch jetz
t kon
kre
t u
nte
n s
teh
e u
nd
irg
en
detw
as
op
tim
iere
, d
an
n i
st d
as
natü
rlic
h ü
berh
au
pt
nic
ht
rele
van
t. D
a i
st e
s m
ir v
öll
ig e
gal.
Ab
er
es
ist
halt
wir
kli
ch d
ie M
oti
vati
on
. W
en
n i
ch m
ich
da u
m jed
es
Pro
zen
t A
OM
[A
ku
stoop
tisc
her
Mod
ula
tor]
Effi
zien
z d
a h
infr
iem
el,
dan
n s
ag
e i
ch m
ir o
k,
dass
mu
ss i
ch jetz
tm
ach
en
. D
as
kost
et
jetz
t vi
ell
eic
ht
ein
en
Tag
, d
am
it d
an
n u
nse
r E
xperi
men
t d
an
nvi
ell
eic
ht
in e
inem
Mon
at
rich
tig
gu
t fu
nkti
on
iert
, w
eil
ich
mic
h d
an
n e
infa
chd
ara
uf
verl
ass
en
kan
n.
Un
d w
en
n d
as
Exp
eri
men
t fu
nkti
on
iert
kan
n i
ch d
as
un
dd
as
mach
en
un
d v
iell
eic
ht
die
Fra
ge b
ean
twort
en
. E
s is
t ein
fach
wir
kli
chM
oti
vati
on
un
d w
as
ein
en
eig
en
tlic
h i
nte
ress
iert
. A
lso m
ich
in
tere
ssie
rt n
ich
t, d
ass
die
AO
M E
ffizi
en
z 4
6 o
der
47
Pro
zen
t err
eic
ht.
Es
ist
halt
bess
er
wen
n e
s 4
7P
roze
nt
sin
d.
74
.
Rein
hard
Das
sin
d d
ie E
rford
ern
isse
.7
5.
Wit
lef
Als
o k
on
kre
t, w
en
n i
ch d
a u
nte
n ü
ber
Vers
chrä
nku
ng
nach
den
ken
wü
rde o
der
üb
er
Dekoh
äre
nzm
od
ell
e o
der
mir
ein
e L
ösu
ng
üb
erl
eg
en
wü
rde,
kön
nte
ich
nic
ht
just
iere
n.
Als
o i
ch n
ich
t. I
ch g
lau
be e
s w
äre
au
ch e
twas
trau
rig
, od
er?
Wen
n m
an
sich
da u
nte
n [
das
Lab
or
ist
im K
ell
er]
ein
fach
hin
stell
t, r
um
just
iert
, ru
mm
ach
tu
nd
jetz
t n
ich
t w
eiß
wofü
r od
er
waru
m.
Man
hätt
e jetz
t n
ich
t ein
Zie
l. D
a k
an
nst
du
jed
en
da u
nte
n h
inst
ell
en
. E
s w
äre
völl
ig W
urs
t. E
s is
t ja
nu
r ein
fach
Han
dw
erk
szeu
g w
as
man
halt
lern
en
mu
ss.
76
.
Rein
hard
Als
o f
ür
mic
h d
as
Sp
an
nen
de a
m E
xperi
men
tiere
n i
st,
dass
du
die
Pall
ett
e v
on
theore
tisc
hen
Notw
en
dig
keit
en
un
d..
.7
7.
Wit
lef
Das
gib
ts b
ei
Th
eore
tikern
au
ch.
Mark
us
[Asp
elm
eye
r] m
ein
t es
gib
t zw
ei
Sort
en
von
Th
eore
tikern
. D
ie E
inen
die
ein
en
Ham
ilto
nia
n [
Ham
ilto
nop
era
tor
: Z
eit
- u
nd
En
erg
ieen
twic
klu
ng
ein
es
Sys
tem
s] h
insc
hre
iben
, n
ich
t d
arü
ber
nach
den
ken
. U
nd
die
An
dere
n d
ie h
alt
darü
ber
nach
den
ken
. W
en
n m
al
halt
nic
ht
darü
ber
nach
den
kt,
ist
es
das
gla
ub
e i
ch n
ich
t. D
u s
chre
ibst
es
hin
un
d ü
berl
eg
st d
ir w
as
bed
eu
tet
das
jetz
t. A
lso e
ben
so w
ie V
ers
chrä
nku
ng
, w
en
n i
ch h
ier
ein
en
nic
ht
sep
era
ble
nZ
ust
an
d h
insc
hre
ibe [
all
g.
Defi
nit
ion
von
Vers
chrä
nku
ng
], a
ber
was
heiß
t d
as
jetz
t,au
f w
as
refe
ren
ziert
es.
Un
d d
as
mach
t h
alt
au
ch e
inen
gu
ten
Th
eore
tiker
au
s u
nd
wah
rsch
ein
lich
ist
es
bei
ein
em
gu
ten
Exp
eri
men
tato
r g
en
au
das
Gle
ich
e.
Wen
n e
rd
a d
rin
ste
ht
un
d h
eru
mju
stie
rt,
üb
erl
eg
t er
sich
wie
kan
n i
ch d
as
verb
ess
ern
od
er
wen
n d
as
ist
was
kan
n i
ch d
am
it m
ach
en
od
er
erg
ibt
das
was
neu
es.
78
.
Rein
hard
Im E
nd
eff
ekt
seh
e i
ch d
as
als
Vora
uss
etz
un
g f
ür
die
Ph
ysik
, w
eil
fast
bei
jed
em
math
em
ati
sch
en
An
sch
reib
en
od
er
so w
as,
du
irg
en
dw
an
n z
u e
inem
Pu
nkt
kom
men
mu
sst,
wo d
u d
an
n n
ach
Bed
eu
tun
g,
od
er
was
es
nu
n w
irkli
ch h
eiß
en
soll
frag
en
mu
sst.
Das
mu
ss m
an
nic
ht
heru
nte
rbre
chen
bis
zu
ein
em
Exp
eri
men
t.A
ber
die
Fra
ge i
st w
as
der
Ham
ilto
nia
n n
un
jetz
t w
irkli
ch m
ein
en
soll
.
79
.
En
twic
klu
ng
Rein
hard
Die
Fra
ge i
st a
uch
wie
die
Gesc
hic
hte
weit
erg
eh
t. A
lso e
s sc
hein
t kla
r zu
sein
wie
die
En
twic
klu
ng
in
[d
iese
m B
ere
ich
, op
t-m
ech
. S
yste
me]
weit
erg
eh
t?8
0.
Wit
lef
Als
o i
ch k
an
n jetz
t ers
tmal
kon
kre
t b
ei
un
s b
leib
en
. Ic
h h
off
e d
as
wir
es
ers
tmal
sch
aff
en
die
Mech
an
ik m
it L
ich
t zu
vers
chrä
nken
. A
lso i
ch d
en
ke d
as
geh
td
efi
nit
iv.
Es
wir
d h
alt
wah
rsch
ein
lich
kn
ap
p s
ein
, ein
fach
au
s te
chn
isch
en
Grü
nd
en
. U
nd
dan
n h
off
e i
ch,
dass
bei
Nik
ola
i's
[Kie
sel]
Exp
eri
men
t m
it d
en
Nan
o-S
ph
äh
ren
, d
ass
die
halt
weit
erk
om
men
als
wir
. D
ass
die
halt
sch
aff
en
so e
ine
Nan
osp
häre
in
ein
e S
up
erp
osi
tion
von
zw
ei
Ort
en
zu
bri
ng
en
un
d d
an
n w
irkli
ch s
oein
e A
rt D
op
pels
palt
exp
eri
men
t zu
mach
en
. U
nd
dan
n w
ird
es,
gla
ub
e i
ch,
ein
fach
sch
wie
rig
in
die
se R
eg
imes
zu k
om
men
, w
o m
an
halt
gen
au
solc
he
Dekoh
äre
nzm
od
ell
e t
est
en
kan
n.
Inw
iew
eit
eb
en
Gra
vita
tion
au
f S
up
erp
osi
tion
en
od
er
so e
ine K
oh
äre
nz
zwis
chen
den
vers
chie
den
en
Zu
stän
den
ein
wir
kt.
Es
ist
tota
l sc
hw
er
zu s
ag
en
. Z
ur
Zeit
kan
n m
an
es
verg
ess
en
. D
as
hat
der
Rain
er
[Kalt
en
baek]
au
sgere
chn
et.
D.h
. er
hat
sich
ein
Exp
eri
men
t ü
berl
eg
t w
as
man
im
Welt
rau
m m
ach
en
kan
n,
weil
da h
alt
das
Vaku
um
bess
er
ist,
weil
es
bess
er
isoli
ert
ist.
Un
d d
a k
om
men
Zah
len
rau
s d
ie g
eh
en
heu
tzu
tag
e n
och
nic
ht.
Un
d d
as
ist
halt
sch
ad
e,
ab
er
es
heiß
t ja
nic
ht
das
es
üb
erh
au
pt
nic
ht
geh
t.
81
.
Rein
hard
Ab
er
es
gib
t zu
min
dest
die
Ric
htu
ng
vor.
82
.W
itle
fW
en
n m
an
sic
h e
ben
mit
die
sen
Sach
en
besc
häft
igt,
zu
m B
eis
pie
l m
it s
o e
iner
exp
eri
men
tell
en
Fra
gest
ell
un
g w
ie i
ch d
as
um
setz
en
kan
n,
un
d d
an
n g
eh
ts h
alt
ein
mal
nic
ht.
Dan
n k
rieg
t m
an
ab
er
ein
e a
nd
ere
Id
ee w
as
man
vie
lleic
ht
an
ders
test
en
kan
n o
der
ob
es
an
dere
s E
xperi
men
t g
ibt
in d
ie R
ich
tun
g.
Un
d i
ch d
en
ke
sch
on
, d
ass
man
irg
en
dw
ie i
n s
o e
inen
Bere
ich
kom
mt,
vie
lleic
ht
in d
en
näch
sten
zeh
n J
ah
ren
, w
o m
an
es
halt
wir
kli
ch s
chaff
t so
lch
e M
od
ell
e z
u t
est
en
. A
lso d
as
wäre
gla
ub
e i
ch w
irkli
ch e
in Z
iel.
Ich
mein
e d
as
träg
t je
tzt
au
ch n
ich
t zu
m..
. Ic
hm
ein
e V
ers
chrä
nku
ng
wir
d m
an
nie
vers
teh
en
kön
nen
, w
ürd
e i
ch m
al
sag
en
. W
ied
u s
chre
ibst
, w
en
n m
an
dam
it a
ufw
äch
st, m
it L
okali
tät
un
d R
eali
smu
s. E
in B
ab
yso
erz
ieh
t, d
ass
halt
all
es
imm
er
da i
st a
uch
wen
n i
ch n
ich
t h
ing
uck
e u
nd
ja w
en
nic
h h
alt
hie
r w
as
tun
kan
n,
dass
dort
nic
ht
sofo
rt b
eein
flu
sst
wir
d,
natü
rlic
h d
an
n
83
.
C Transcription of Interviews
118
kan
n m
an
das
nic
ht
vers
teh
en
; n
ie.
Es
ist
halt
au
ch s
o,
wen
n m
an
irg
en
dw
an
nd
urc
h e
in S
TM
[R
ast
ert
un
nelm
ikro
skop
, sc
an
nin
g t
un
neli
ng
mic
rosc
op
e]
du
rch
sch
au
t od
er
ein
e O
berfl
äch
e a
tom
au
flöst
, d
as
kan
n m
an
au
ch n
ich
tvo
rste
llen
. D
as
sieh
t m
an
halt
un
d g
lau
bt,
dass
das
so a
uss
ieh
t.R
ein
hard
Ja,
ab
er
das
Pro
ble
m i
st.
Man
sie
ht
gera
de d
iese
Ku
gerl
n o
der
Halb
ku
geln
un
dm
an
kom
mt
nie
um
hin
die
als
eb
en
solc
he K
ug
erl
n [
soli
de S
ph
äre
n]
zu s
eh
en
.S
chau
t m
an
sic
h a
n w
ie d
iese
ST
M u
nd
die
an
dere
n S
ach
en
fu
nkti
on
iere
n,
so s
ind
es
in d
em
Sin
n n
ur
En
erg
ieau
fzeic
hn
un
gen
[M
ess
un
gen
von
En
erg
ie e
ines
best
.S
chw
ell
en
wert
es]
.
84
.
Wit
lef
Ab
er,
da w
ürd
e i
ch a
ntw
ort
en
. O
k,
das
sch
aff
t m
an
sic
herl
ich
au
ch,
in f
ün
f b
is z
eh
nJa
hre
n,
dass
man
ein
e V
ers
chrä
nku
ng
qu
ell
e b
au
t, d
ie a
us
meh
rere
n P
hoto
nen
best
eh
t, d
ass
man
halt
wir
kli
ch m
it s
ein
en
eig
en
en
Au
gen
die
Mess
un
g m
ach
t. D
as
man
sic
h,
was
weiß
ich
, Pola
risa
tion
sfilt
er
davo
r m
ach
t. H
ier
ein
Kli
ck,
da e
inK
lick
, kli
ck k
lick
kli
ck.
Das
man
es
halt
mit
sic
h s
elb
st m
ach
t so
ein
Exp
eri
men
t.U
nd
dan
n e
ine S
tric
hli
ste u
nd
sie
ht
[die
Vers
chrä
nku
ng
].
85
.
Rein
hard
Die
se V
ers
chrä
nku
ng
sexp
eri
men
te d
ie e
s g
ibt,
die
es
au
ch i
n d
er
Au
sbil
du
ng
usw
.g
ibt,
die
hab
en
sch
on
ein
e e
rsch
reck
en
de E
infa
chh
eit
un
d,
für
mic
h z
um
ind
est
,[Ü
berz
eu
gu
ng
skra
ft].
Es
ist
halt
im
mer
nu
r d
iese
r Ü
berg
an
g s
chw
er
zub
eg
rün
den
, b
zw.
sch
wer
zu b
eh
au
pte
n,
weil
er
geg
en
etw
as
spri
cht
was
man
imm
er
an
nim
mt.
[N
äm
lich
], d
ass
es
mit
lokalr
eali
stis
chen
Sach
en
eb
en
nic
ht
geh
t.A
lso,
dass
die
Korr
ela
tion
un
d V
ers
chän
ku
ng
da i
st,
das
kan
n m
an
eig
en
tlic
hzi
em
lich
üb
erz
eu
gen
d d
ars
tell
en
. A
ber,
dass
es
dam
it n
ich
t erk
lärb
ar
ist.
Un
d d
ais
t fü
r m
ich
im
mer
au
ch d
er
Sp
run
g w
o m
an
sic
h h
alt
im
mer
selb
st d
azu
bri
ng
en
mu
ss.
Das
man
sag
t ok,
ich
bin
jetz
t ü
erz
eu
gt
word
en
von
Bell
usw
., d
ass
es
lokalr
eali
stis
ch n
ich
t lä
uft
un
d a
ls r
ati
on
all
es
Kon
stru
kt,
od
er
wie
im
mer
man
sag
en
wil
l, s
eh
e d
avo
n a
b f
ür
all
e m
ein
e w
eit
ere
n D
ing
e d
ie i
ch i
n d
em
Bere
ich
mach
e,
d.h
. fü
r d
ie g
an
zen
Exp
eri
men
te u
sw.
Es
ist
ab
er
die
Fra
ge w
ie w
eit
das
"natü
rlic
h"
sein
kan
n,
od
er
selb
stve
rstä
nd
lich
.
86
.
Wit
lef
Ab
er,
das
weiß
t d
u w
ah
rsch
ein
lich
vie
l b
ess
er
was
man
natü
rlic
h u
nd
selb
stve
rstä
nd
lich
heiß
t. I
st d
as
nic
ht
ein
e F
rag
e d
er
Erz
ieh
un
g,
als
o e
ine F
rag
ed
er
Au
sbil
du
ng
. O
der
ein
e F
rag
e,
dass
es
gar
nic
ht
geh
t, w
eil
man
au
fwäch
st m
itg
reif
en
, an
fass
en
un
d s
o?
87
.
Rein
hard
Ab
er
du
bis
t ja
jetz
t lä
ng
er
in d
em
Feld
wie
ich
au
f je
den
Fall
. E
s g
ibt
sch
on
ein
eg
ew
isse
Selb
stve
rstä
nd
lich
keit
im
Um
gan
g m
it d
en
Din
gen
.8
8.
Wit
lef
Ja k
lar
mit
Vers
chrä
nku
ng
, D
efi
nit
ion
en
un
d s
o.
Ein
e E
rklä
run
g h
ab
e i
ch t
rotz
dem
nic
ht.
Ich
kan
ns
au
ch n
ur
so e
rklä
ren
, d
ass
lokale
r R
eali
smu
s ein
fach
nic
ht
dam
itein
herg
eh
t.
89
.
Rein
hard
Die
se P
rob
lem
ati
k s
chie
bt
sich
dan
n e
twas
rau
s, w
eil
im
täg
lich
en
Gesc
häft
...
Od
er
wü
rdest
du
das
nic
ht.
..?
90
.
Wit
lef
Als
o i
m t
äg
lich
en
Gesc
häft
bra
uch
e i
ch e
s h
alt
nic
ht,
ab
er
die
Pro
ble
mati
k i
st ja
trotz
dem
da.
Die
geh
t n
ich
t ve
rlore
n.
Die
ist
da.
D.h
. je
tzt
nic
ht
das
ich
au
fhöre
nw
ürd
e z
u a
rbeit
en
, w
eil
ich
das
ers
tmal
löse
n w
ill.
Son
dern
sie
ist
ein
fach
da u
nd
un
gelö
st.
Wie
gesa
gt,
es
geh
t n
ur
du
rch
ein
e n
eu
e T
heori
e,
das
irg
en
dw
ieau
fzu
löse
n.[
Pau
se]
Wen
n e
s au
flösb
ar
ist.
Wen
n m
an
es
nic
ht
ein
fach
akze
pti
ere
nm
uss
.
91
.
Rein
hard
Ja d
as
ist
die
Fra
ge.
Es
gib
t g
en
ug
Leu
te,
au
ch P
hys
iker
usw
., d
ie [
Letz
tere
sm
ein
en
]. D
ie s
tell
en
au
ch d
ie F
rag
e w
ie r
ele
van
t d
an
n a
uch
solc
he D
isku
ssio
nen
sin
d.
Das
wil
l ic
h s
ow
ieso
nu
r an
stoss
en
.
92
.
Wit
lef
Es
ist
ein
bis
sch
en
sch
wie
rig
, w
eil
es
halt
ein
Th
em
a i
st,
dass
seit
jü
nfz
ig J
ah
ren
,se
it B
ell
, in
best
imm
ten
Kre
isen
dis
ku
tiert
wir
d.
Seit
zw
an
zig
Jah
ren
ist
es
wah
rsch
ein
lich
so,
da i
st a
m B
est
en
den
An
ton
[Z
eil
ing
er]
mal
zu f
rag
en
od
er
den
Mark
us
[Asp
elm
eye
r] d
er
weiß
das
sich
erl
ich
au
ch,
dass
es
au
ch w
en
n m
an
sic
hd
arü
ber
un
terh
ält
nic
ht
der
Tod
sein
er
Karr
iere
ist
. W
eil
es
nic
ht
etw
as
ist,
was
eso
teri
sch
ist
. E
s w
ird
ja a
ls P
rob
lem
erk
an
nt
un
d a
uch
als
wic
hti
g.
Un
d s
eit
zeh
nJa
hre
n,
viell
eic
ht
ein
bis
sch
en
meh
r, i
st d
urc
h d
ie Q
uan
ten
info
rmati
on
ein
völl
igan
dere
r A
spekt
noch
mal
dazu
gekom
men
. D
as
nic
ht
nu
r eso
teri
sch
ist
od
er
halt
nu
rein
Pro
ble
m d
er
Ph
ysik
, so
nd
ern
, d
ass
man
dam
it a
uch
etw
as
mach
en
kan
n.
Un
dw
ah
rsch
ein
lich
hat
es
dem
, se
it m
an
mit
der
Vers
chrä
nku
ng
was
mach
en
kan
n,
au
ch w
ah
nsi
nn
ig g
eh
olf
en
. D
ass
man
au
ch n
ich
t n
ur
jetz
t d
am
it w
as
mach
en
kan
n,
son
dern
au
ch m
al
wie
der
frag
en
vers
teh
e i
ch v
iell
eic
ht
ein
e E
rklä
run
g o
der
fin
de
ein
en
an
dere
n Z
ug
an
g.
93
.
Rein
hard
Die
Mög
lich
keit
en
, exp
eri
men
tell
, h
ab
en
sic
h s
eh
r g
ew
eit
et.
Da i
st e
s kla
r d
as
au
ch d
ie F
rag
e w
ied
er
aku
t w
erd
en
kan
n.
94
.
Wit
lef
Es
ist
halt
ein
fach
ein
un
gelö
stes
Pro
ble
m,
für
mic
h.
Man
weiß
sozu
sag
en
, d
ass
lokale
r R
eali
smu
s u
nd
voll
stän
dig
e Q
uan
ten
mech
an
ik g
eh
t n
ich
t m
itVers
chrä
nku
ng
ein
her.
Un
d e
s g
ibt
kein
e L
ösu
ng
smög
lich
keit
en
. W
as
halt
span
nen
d w
äre
irg
en
dw
ie m
al,
...
ok l
etz
ten
dli
ch s
ind
es
halt
solc
he
Un
gle
ich
un
gen
. D
ass
man
sic
h ü
berl
eg
t, d
as
un
d d
as
au
fgeb
e,
da g
ibt
es
gan
zeB
üch
er
dazu
, g
ibt
es
ein
e e
xperi
men
tell
e K
on
seq
uen
z d
ara
us
die
ich
halt
üb
erp
rüfe
n k
an
n.
Ab
er
wah
rsch
ein
lich
sin
d e
s d
ie g
an
zen
Un
gle
ich
un
gen
die
da
rum
geis
tern
. E
s w
är
mal
span
ned
irg
en
dw
ie w
as
an
dere
s zu
hab
en
als
ein
eU
ng
leic
hu
ng
im
mer
zu m
ess
en
. D
ass
man
mal
ein
e p
hys
ikali
sch
e K
on
seq
uen
z h
at.
Wen
n i
ch h
alt
Lokali
tät,
...
Das
Pro
ble
m i
st ja a
uch
, es
wäre
ja n
ich
t so
ein
eL
okali
tät
die
man
au
fgib
t, d
ass
man
au
f ein
mal
mit
Üb
erl
ich
tgesc
hw
ind
igkeit
Sig
nale
üb
ert
rag
en
kan
n.
95
.
Rein
hard
Die
s W
ürd
e d
an
n w
ied
er
ein
e L
okali
tät,
od
er
Beg
riff
bed
eu
ten
, d
er.
..9
6.
Wit
lef
Kau
sali
tät
in d
em
Sin
ne m
uss
man
nic
ht
au
fgeb
en
. S
ag
en
wir
es
mal,
dass
man
irg
en
dw
ie n
och
was
an
dere
s...
ein
en
ph
ysik
ali
sch
en
Eff
ekt
den
man
test
en
kan
n.
Ab
er
da k
en
ne i
ch m
ich
au
ch z
u s
chle
cht
au
s.
97
.
Was
ich
vorh
er
noch
sag
en
woll
te,
weil
du
gem
ein
t h
ast
von
weg
en
sp
an
ned
. W
as
au
ch n
och
tota
l sp
an
nen
d fi
nd
e,
was
au
ch b
ei
Vers
chrä
nku
ng
im
pli
zit
dri
n i
st,
ab
er
jetz
t n
ich
t u
nb
ed
ing
t so
herv
ort
ritt
. A
lso s
ag
en
wir
es
wir
d n
ich
t th
em
ati
siert
, d
ass
ein
fach
wen
n e
in F
est
körp
er,
zu
m B
eis
pie
l in
jü
ng
ster
Zeit
irg
en
dw
ie a
lles
irg
en
dw
ie v
ers
chrä
nkt.
Eb
en
gera
de d
ie E
xperi
men
te m
it o
pti
sch
en
Git
tern
, w
od
ie A
tom
e s
o e
inze
ln p
lazi
ert
sin
d.
Die
hab
en
es
gesc
haff
t ein
zele
ne A
tom
e z
uad
dre
ssie
ren
un
d d
ass
man
dam
it h
alt
Fest
körp
ers
yste
me m
ög
lich
st s
imu
liere
nkan
n.
Un
d v
iell
eic
ht
es
au
ch s
chaff
t d
ie S
up
rale
itu
ng
, H
och
tem
pera
tur-
Su
pra
leit
un
g,
zu e
rklä
ren
. O
der
ein
fach
irg
en
dw
elc
he P
hän
om
en
e,
die
man
im
Fest
körp
er
dre
ckig
hin
kri
eg
t, h
alt
wah
nsi
nn
ing
sau
ber
hin
zukri
eg
en
. D
as
fin
d i
chto
tal
span
nen
d.
Da i
st V
ers
chrä
nku
ng
im
pli
zit
ein
fach
da.
Es
wir
d e
ben
in
dem
Sin
ne n
ich
t p
hil
oso
ph
isch
th
em
ati
siert
, so
nd
ern
es
wir
d e
infa
ch a
usg
en
utz
t,u
nte
rsu
cht.
98
.
119
Rein
hard
Ab
er
das
wäre
dan
n s
ozu
sag
en
der
Üb
erg
an
g d
an
n v
on
der
qu
an
ten
mech
an
isch
en
Seit
e z
u e
iner
kla
ssic
hen
Sach
e,
od
er
zu g
röß
ere
n S
yste
men
. W
en
n d
u s
ag
stS
up
rale
itu
ng
od
er
grö
ßere
Fest
körp
er,
...
99
.
Wit
lef
Ja k
lar.
Letz
ten
dli
ch i
st S
up
rale
itu
ng
au
ch e
in m
akro
skop
isch
er
Qu
an
ten
eff
ekt.
Wo
du
halt
au
ch e
ine W
ell
en
fun
kti
on
hin
sch
reib
st d
ie v
ers
chrä
nkt
ist.
Als
o w
ill
ein
fach
nu
r sa
gen
, V
ielt
eil
chen
eff
ekte
sin
d a
uch
wah
nsi
nn
ig s
pan
nen
d.
10
0.
Rein
hard
Weil
du
dan
n d
iese
n Ü
berg
an
g b
ess
er,
der
sch
ein
t ir
gen
dw
ie t
heore
tisc
h n
ur
post
uli
ert
zu
sein
, [v
ers
teh
en
wir
st k
ön
nen
]. D
as
die
s vo
rhan
den
ist
kan
n m
an
irg
en
wie
mach
en
...
10
1.
(no s
peaker)
[ku
rze U
nte
rbre
chu
ng
du
rch
Koll
eg
en
]1
02
.
Off
en
e F
rag
en
?
Rein
hard
Im E
nd
eff
ekt
wäre
es
das
[gew
ese
n].
Die
Fra
ge i
st o
b d
u n
och
Fra
gen
hätt
est
,w
en
n d
u s
chon
vorb
ere
itet
bis
t [d
.h.
mein
Exp
ose
gele
sen
hast
]? [
Dan
ksa
gu
ng
un
dku
rzes
pers
ön
lich
es
Gesp
räch
.]
10
3.
C Transcription of Interviews
120
Jon
as_
110622
Inte
rvie
w m
it J
on
as
Hörs
ch v
om
22
.06
.20
11
Tra
nsc
rib
ed
by
yott
a,
vers
ion
2 o
f 1
10
63
0
An
fan
g,
pers
ön
lich
e D
ate
n,
Au
sbil
du
ng
(no s
peaker)
[in
tro s
mall
talk
]1
.R
ein
hard
Am
An
fan
g w
ill
ich
eig
en
tlic
h n
ur
all
gm
ein
es
wis
sen
. W
ie a
lt b
ist
du
?2
.Jo
nas Ic
h b
in 2
5.
Ja,
gen
au
. M
uss
te e
s ab
er
nach
rech
nen
.3
.R
ein
hard
Das
mü
ssen
zie
mli
ch v
iele
Leu
te.
4.
Jon
as Ic
h m
erk
e m
ir h
alt
85
. G
en
au
.5
.R
ein
hard
Kan
nst
du
mir
sag
en
, u
ng
efä
hr
dein
e A
usb
ild
un
g,
jetz
t st
ud
en
tisc
h?
6.
Jon
as G
en
au
, ic
h b
in n
och
Stu
den
t. I
ch h
ab
e jetz
t...
An
sic
h h
ab
e i
ch n
ur
Ph
ysik
eb
en
in
Deu
tsch
lan
d s
tud
iert
. B
in jetz
t ir
gen
dw
ie b
ei
der
Dip
lom
arb
eit
sph
ase
.7
.
Rein
hard
Un
d w
o?
8.
Jon
as In
Pots
dam
. U
nd
sch
reib
jetz
t eig
en
tlic
h i
n P
ots
dam
mein
e D
iplo
marb
eit
un
d d
as
ist
ab
er
so e
ine K
oll
ab
ora
tion
zw
isch
en
Jen
s E
isert
[h
ttp
://w
ww
.jen
se.q
ipc.
org
/Main
Pag
e.h
tml]
un
d h
ier
Mark
us
Asp
elm
eye
r. U
nd
dan
n s
oll
ich
zw
isch
en
den
Beid
en
ein
bis
sch
en
sp
rin
gen
. Je
tzt
bin
ich
halt
die
ers
te H
älf
te,
hab
e i
ch jetz
tg
esa
gt,
bin
ich
grö
ßte
nte
ils
hie
r. W
eil
wir
hie
r n
och
das
Teil
bau
en
mü
ssen
, w
as
wir
dan
n i
rgew
an
n f
rüh
er
od
er
späte
r au
ch n
och
mach
en
.
9.
Rein
hard
Ah
ok.
Un
d d
u h
ast
dan
n e
igen
tlic
h n
ur
norm
ale
Sta
nd
ard
-Ph
ysik
au
sbil
du
ng
gem
ach
t?1
0.
Jon
as Ja
, g
en
au
. H
ab
nu
r ein
Dip
lom
Ph
ysik
gem
ach
t.1
1.
Rein
hard
Un
d d
ein
e D
iplo
marb
eit
ist
üb
er.
..?
12
.
Dip
lom
arb
eit
Jon
as M
ein
e D
iplo
marb
eit
ist
...
Das
blö
de i
st,
wir
hab
en
noch
kein
en
Nam
en
, d
esw
eg
en
kan
n i
ch d
as
nic
ht
irg
en
dw
ie k
urz
ben
en
nen
. A
ber
an
sic
h s
ind
es
irg
en
dw
ie s
o...
Ich
weiß
nic
ht
ob
dir
ein
e C
avi
ty i
rgen
dw
as
sag
t.
13
.
Rein
hard
Ja,
ja.
14
.Jo
nas Zw
ei
Mic
ro-C
avi
ties
die
mit
ein
er
mech
an
isch
en
Brü
cke m
itein
an
der
gekop
pelt
15
.
sin
d.
Man
kan
n b
eid
e C
avi
ties
mit
Lase
r an
spre
chen
, so
dass
dan
n w
en
n m
an
pra
kti
sch
die
Ein
e d
an
n a
nre
gt,
dan
n w
ird
sic
h ü
ber
die
se m
ech
an
isch
e K
op
plu
ng
,w
ird
sic
h d
as
eb
en
au
ch a
uf
den
An
dere
n a
usü
ben
. U
nd
wir
woll
en
jetz
t sc
hau
en
was
wir
dam
it m
ach
en
kön
nen
. B
zw.
was
man
da m
ach
en
kan
n w
en
n m
an
dre
ißig
solc
her
Teil
e h
inte
rein
an
der
hat,
ob
man
da i
rgen
welc
he T
ran
sport
eff
ekte
sie
ht.
Ich
mach
e d
en
th
eore
tisc
hen
Part
dazu
, u
nd
dan
n s
oll
dass
woh
l G
arr
ett
[C
ole
] so
bau
en
un
d ü
berp
rüfe
n,
was
dab
ei
rau
skom
mt.
Rein
hard
Als
o d
ein
Teil
ist
eh
er
der
theore
tisc
he..
.1
6.
Jon
as G
en
au
. Ic
h s
oll
s m
al
du
rch
rech
nen
.1
7.
Rein
hard
D.h
. au
ch s
imu
liere
n d
as
Teil
? O
der
ist
das
nu
r...
?1
8.
Jon
as A
lso w
ir h
ab
en
ein
bis
sch
en
was.
.. W
ir h
ab
en
die
mech
an
isch
en
Eig
en
sch
aft
en
von
so e
inem
Din
gen
.. h
ab
en
wir
sim
uli
ert
. A
ber
mit
ein
er
Sta
nd
ard
soft
ware
. D
as
sin
dd
iese
Fin
ite-E
lem
en
t-S
olv
er,
heiß
en
die
. G
en
au
, d
a h
ab
en
wir
das.
.. D
a h
ab
en
wir
die
Str
uktu
r eb
en
erz
eu
gt
un
d h
ab
en
dan
n g
esc
hau
t, w
as
rech
net
er
un
s d
en
n f
ür
Eig
en
wert
e a
us.
Das
war
was
wir
gem
ach
t h
ab
en
, ab
er
son
st s
imu
liere
n..
. K
ein
eA
hn
un
g,
ich
werd
e a
b u
nd
an
ein
e D
iffere
nti
alg
leic
hu
ng
irg
en
dw
ie n
um
eri
sch
halb
weg
s lö
sen
mü
ssen
. D
a i
st n
och
nic
ht
viel
pass
iert
.
19
.
Rein
hard
Ok.
Wo b
ist
du
da u
ng
efä
hr
jetz
t?2
0.
Jon
as Ic
h h
ab
gera
de e
rst
an
gefa
ng
en
. Vor
ein
ein
halb
Mon
ate
n o
der
zwei
Mon
ate
n.
Ich
bin
noch
in
sow
as
wie
der
Ein
lese
ph
ase
un
d h
ab
sch
on
das
ein
e o
der
an
dere
sch
on
mal
vorg
em
ach
t. A
ber
eig
en
tlic
h s
am
mle
ich
im
mer
noch
. E
igen
tlic
h h
ab
ich
bis
her
blo
ß s
tud
iert
.
21
.
Rein
hard
Au
fwen
dig
gen
ug
. D
.h.
un
gefä
hre
r Z
eit
pla
n,
wie
das
lau
fen
soll
?2
2.
Jon
as N
äch
sten
Ap
ril,
näch
sten
Mai
wü
rde i
ch g
ern
e a
bg
eb
en
.2
3.
Rein
hard
D.h
. so
ein
Jah
r g
ep
lan
t.2
4.
Jon
as G
en
au
, ein
Jah
r in
sgesa
mt
ist
gep
lan
t.2
5.
Rein
hard
Un
d h
alt
au
fgete
ilt,
wie
du
gesa
gt
hast
, ein
Teil
hie
r, e
in T
eil
in
...?
26
.Jo
nas Ja
. A
ber
es
ist
üb
erh
au
pt
nic
ht
fest
gesc
hri
eb
en
was
wo i
st.
Irg
en
dw
ie w
ar
mein
Pro
fess
or
in P
ots
dam
dan
n i
rgen
dw
an
n,
als
mit
sein
er
[???
?],
bin
jetz
t n
ach
Wie
nu
mg
ezo
gen
wie
gep
lan
t w
ar,
mein
te e
r: A
ha,
ich
hab
das
nic
ht
so g
ep
lan
t. W
irh
ab
en
das
eig
en
tlic
h n
ich
t so
gen
au
fest
gele
gt,
ab
er
ja i
st g
ut.
Na ja,
in m
ein
em
eig
en
en
erm
ess
en
so w
ie e
s au
ssie
ht,
wo i
ch g
era
de l
ieb
er
bin
od
er
so.
27
.
Rein
hard
Od
er
was
halt
fü
r d
ie A
rbeit
irg
en
dw
ie..
.?2
8.
Jon
as G
en
au
. G
era
de b
in i
ch f
ast
der
Mein
un
g,
dass
es
fast
sin
nvo
ller
wäre
in
Pots
dam
.W
eil
da k
ön
nte
ich
jetz
t m
eh
r th
eore
tisc
he F
rag
en
ste
llen
. Je
tzt
ist
irg
en
dw
ie d
er
exp
eri
men
tell
e T
eil
so h
alb
weg
s an
gest
oss
en
, od
er
sow
as.
Das
da e
in b
issc
hen
was
pass
iert
, w
o i
ch jetz
t so
wie
so g
era
de k
ein
en
Ein
flu
ß n
eh
men
kan
n f
ür
die
näch
sten
ein
ein
halb
, zw
ei
Mon
ate
. U
nd
eig
en
tlic
h w
ärs
dan
n s
inn
voll
er
in P
ots
dam
zu
sein
,
29
.
121
wo i
ch m
eh
r F
rag
en
ste
llen
kan
n,
zum
ind
est
zu
irg
en
dw
as.
Ich
hab
kein
en
Pla
n.
Rein
hard
Als
o d
as
heiß
t d
u b
ist
hie
rher
gekom
men
um
dir
ein
mal
das
Exp
eri
men
tell
ean
zusc
hau
en
? W
as
hie
r g
eh
t.3
0.
Jon
as G
en
au
, u
m m
ir d
as
an
zusc
hau
en
. U
nd
fü
r d
as
mech
an
isch
e Z
eu
gs,
wie
man
das
sim
uli
ert
. D
a k
an
nte
n s
ich
die
hie
r vi
el
bess
er
au
s, w
eil
die
das
halt
fü
r ih
reE
xperi
men
te v
orh
er
ku
rz m
ach
en
. U
nd
dan
n s
chau
en
was
pass
iert
. D
esw
eg
en
hab
e i
ch d
as
eb
en
hie
r g
em
ach
t. U
nd
eig
en
tlic
h i
st d
as
jetz
t ers
tmal
so,
dass
er
[Garr
ett
Cole
] so
die
ers
ten
Teil
e b
au
t m
it d
en
en
er
was
pro
bie
ren
wil
l. U
nd
dan
nkri
eg
ich
halt
irg
en
dw
an
n d
ie D
ate
n.
31
.
Rein
hard
Als
o d
er
Garr
ett
[C
ole
] b
au
t d
ie..
.?3
2.
Jon
as G
arr
ett
[C
ole
] m
ach
t d
as
dan
n.
Ich
hab
dam
it s
ofe
rn w
as
zutu
n,
dass
ich
die
Geom
etr
ie i
rgen
dw
ie g
esa
gt
hab
e d
as
wäre
in
tere
ssan
t. A
ber.
..3
3.
Rein
hard
Das
ist
Au
ftra
gsa
rbeit
an
den
Garr
ett
das
zu m
ach
en
.3
4.
Jon
as In
die
Ric
htu
ng
. E
s im
mer
noch
nic
ht
gan
z lo
sgest
oss
en
. A
ber
es
soll
te jetz
tir
gen
dw
an
n m
al
lan
gsa
m k
lap
pen
.3
5.
Rein
hard
Vers
teh
e.
Un
d w
ie b
ist
du
irg
en
dw
ie s
pezi
ell
au
f d
as
Th
em
a g
ekom
men
. O
der,
dass
du
üb
erh
au
pt
in d
en
Bere
ich
geh
st?
36
.
Jon
as Ä
hm
...
Als
o i
ch b
in h
alt
üb
er.
.. A
n s
ich
hab
en
wir
in
Pots
dam
gar
nic
ht
sovi
el
Au
swah
l g
eh
ab
t. U
nd
letz
ten
dli
ch w
ars
dan
n d
er
Pro
fess
or.
Es
war
dan
n h
alt
Jen
sE
isert
, d
er
sein
e Q
uan
ten
info
rmati
on
gem
ach
t h
at.
Un
d e
r h
at
bei
un
s eb
en
au
chein
...
Dre
i Vorl
esu
ng
en
hab
e i
ch i
nzw
isch
en
bei
ihm
geh
ört
. U
nd
die
Vorl
esu
ng
en
ware
n e
igen
tlic
h e
cht
gan
z to
ll,
un
d d
a h
ab
e i
ch m
ich
eb
en
halt
so S
tück
fü
rS
tück
...
Zu
näch
st h
ab
e i
ch G
un
dvo
rlesu
ng
geh
ab
t u
nd
dan
n h
ab
e i
ch m
ich
in
sein
eS
pezi
alv
orl
esu
ng
en
ein
gearb
eit
et
geh
ab
t. U
nd
dan
n b
in i
ch s
o a
uf
die
Qu
an
ten
info
rmati
on
gekom
men
. Q
uan
ten
info
rmati
on
ist
dan
n v
iell
eic
ht
ein
bis
sch
en
zu
wen
ig a
nw
en
du
ng
sbezo
gen
, d
ach
te i
ch d
an
n i
rgen
dw
an
n.
Un
d d
an
nb
in s
o a
uf
die
Op
to-M
ech
an
ik g
ekom
men
, w
o d
an
n a
uch
vie
l Q
uan
ten
info
rmati
on
an
sic
h d
rin
steck
t, a
ber
wo m
an
das
Din
g h
alt
bau
t. O
der
irg
en
dje
man
d b
au
t.
37
.
Rein
hard
Un
d w
ie w
ar
da u
ng
efä
hr
der.
.. W
an
n t
ritt
das
ein
? Ic
h k
en
ne n
ur
hie
r vo
mS
tud
ium
, d
ass
man
da s
o i
rgen
dw
an
n i
n d
er
Mit
te d
an
n s
oQ
uan
ten
mech
an
ikth
eori
e m
ach
t. V
orh
er
nu
r so
en
bis
serl
Au
sbli
cks.
..?
38
.
Jon
as W
ir h
ab
en
im
vie
rten
Sem
est
er
halt
Qu
an
ten
mech
an
ik g
eh
ört
, g
lau
be i
ch..
. Ja
,vi
ert
es
Sem
est
er.
Th
eore
tisc
he.
Das
fan
d i
ch d
am
als
gan
z co
ol
eig
en
tlic
h.
Pro
f w
ar
eig
en
tlic
h n
ich
t so
gu
t. A
ber
doch
war
ein
fach
in
tere
ssan
t, w
eil
da i
rgen
dw
ie g
an
z,g
an
z sk
uri
ll,
gan
z an
ders
war.
Ja u
nd
dan
n d
ach
te i
ch,
irg
en
dw
as
in d
ie R
ich
tun
gw
äre
sch
on
in
tere
ssan
t. O
der
mal
sch
au
en
. D
an
n e
infa
ch h
alt
...
So i
m S
ech
sten
hab
e i
ch d
an
n e
ben
so n
och
neb
en
her
an
gefa
ng
en
Qu
an
ten
info
rmati
on
zu
höre
n.
Sie
bte
s, A
chte
s d
an
n m
eh
r g
eh
ört
un
d e
igen
tlic
h a
nd
ere
Sach
en
fert
ig g
em
ach
t.U
nd
bei
dem
irg
en
dw
ie a
uch
ein
Pro
jekt
gem
ach
t, b
eim
Eis
ert
. G
en
au
, u
nd
so
irg
en
wie
. A
uch
Mit
te w
ürd
e i
ch s
ag
en
au
f d
ie Q
uan
ten
mech
an
ik g
est
oss
en
un
dd
an
n h
alt
irg
en
dw
ie g
eku
ckt
was
es
von
dem
Qu
an
ten
teil
noch
gib
t.
39
.
Rein
hard
Un
d k
an
nst
du
irg
en
dw
ie f
est
mach
en
, w
as
dic
h i
nte
ress
iert
hat?
Als
o g
era
de d
as
zu m
ach
en
? O
der
nu
r so
rein
geru
tsch
t?4
0.
Jon
as E
s is
t ein
bis
sch
en
rein
geru
tsch
t w
ürd
e i
ch s
ag
en
, ab
er
es
war
halt
au
ch e
infa
chir
gen
dw
ie w
as
gan
z an
dere
s. A
lso i
ch h
ab
ku
rz A
llg
em
ein
e R
ela
tivi
täts
theori
ean
geh
ört
, d
as
ist
wir
kli
ch s
chic
k k
on
zep
tion
ell
un
d s
o.
Ab
er
irg
en
wie
kam
's m
ir s
ovo
r w
ie w
en
n m
an
eff
ekti
v n
ich
ts m
ach
en
kan
n.
Weil
es
irg
en
dw
ie z
u k
om
pli
ziert
wir
d,
seh
r sc
hn
ell
. U
nd
irg
en
dw
ie k
an
n m
an
in
der
Qu
an
ten
mech
an
ik d
och
noch
...
Zu
min
dest
all
es
irg
en
dw
ie a
uf
harm
on
isch
e O
szil
lato
ren
zu
rück
füh
ren
un
d d
ied
an
n m
ach
en
. Ja
, p
lus
min
us.
Un
d d
an
n w
ar'
s eb
en
in
tere
ssan
t, w
eil
's a
nd
ers
war.
Un
d a
ber
halt
au
ch m
eis
ten
s n
och
irg
en
dw
ie r
ech
en
bar,
weil
's a
bst
rah
iert
gen
ug
ist.
41
.
Rein
hard
Als
o e
s lä
sst
sich
seh
r, s
eh
r m
inim
ali
stis
ch m
ach
en
. M
it d
en
Osz
illa
tore
n, m
it d
em
harm
on
isch
en
un
d s
o w
eit
er.
Das
ist
sch
on
seh
r...
42
.
Jon
as G
en
au
man
hat
halt
nu
r so
ein
paar
Pri
nzi
pie
n u
nd
wen
n m
an
die
dan
n i
rgen
dw
ieve
rin
nerl
ich
t, k
an
n m
an
eig
en
tlic
h v
iel
mach
en
. D
as
war
inte
ress
an
t.4
3.
Rein
hard
Vers
teh
e.
Un
d,
weil
du
vorh
er
gesa
gt
hast
, w
eil
es
au
ch d
ie M
ög
lich
keit
gib
t d
er
An
wen
du
ng
od
er
zum
ind
est
dam
it e
in b
isse
rl w
as
zu t
un
. W
ie s
ieh
st d
a s
ozu
sag
en
das
Verh
ält
nis
? W
eil
du
ein
ers
eit
s ja
ein
en
th
eore
tisc
hen
Teil
mach
st,
ab
er
doch
zum
ind
est
en
s ja
au
ch h
ier
bis
t u
m d
ie e
xperi
men
tell
en
Sach
en
zu
mach
en
?
44
.
Jon
as U
m d
am
it K
on
takt
zu h
ab
en
. W
ie i
ch d
as
seh
e?
Na ja,
als
o m
an
hat
halt
zu
min
dest
im O
pti
sch
en
...
In d
er
Qu
an
ten
op
tik h
at
man
eb
en
irg
en
dw
ie e
inen
rela
tiv
dir
ekte
nB
ezu
g z
u d
em
gan
zen
Qu
an
ten
zeu
g,
weil
man
sog
ar
als
ein
e P
ers
on
mit
ein
paar
Bau
teil
en
irg
en
dw
ie e
inig
e Q
uan
ten
eff
ekte
sie
ht
un
d b
eob
ach
ten
kan
n.
Un
d d
as
fan
d i
ch a
uch
in
tere
ssan
t. D
as
wär
eig
en
tlic
h d
as
Zw
eit
e g
ew
ese
n w
as
ich
son
stg
em
ach
t h
ätt
e.
Ich
wäre
wah
rsch
ein
lich
in
so e
ine G
rup
pe g
eg
an
gen
bei
un
s in
Pots
dam
, d
ie e
ben
au
ch Q
uan
ten
op
tik m
ach
t. A
lso e
xperi
men
tell
mach
t. A
ber
es
hat
dan
n e
infa
ch n
ich
t so
gu
t g
ep
ass
t. A
ber
gen
au
, d
a w
ar
ein
fach
das
Inte
ress
an
te:
"Ja,
bau
das!
" M
it d
er
rich
tig
en
Au
srü
stu
ng
kan
n d
as
irg
en
dw
ie jed
er
so e
in b
issc
hen
mach
en
. D
as
fan
d i
ch s
pan
nen
d.
Ab
er
jetz
t w
eiß
ich
nic
ht,
ob
es
die
Fra
ge b
ean
twort
et.
45
.
Verh
ält
nis
Th
eori
e -
Exp
eri
men
t
Rein
hard
Die
Fra
ge i
st e
igen
tlic
h:
Waru
m w
ürd
est
du
jetz
t zu
min
dest
en
s d
iese
exp
eri
men
tell
e A
nw
en
du
ng
ben
öti
gen
? D
u k
ön
nte
st ja t
heore
tisc
h d
as
nu
r...
Als
ore
in t
heore
tisc
h m
ach
en
, au
f Pap
ier.
46
.
Jon
as N
a i
rgen
dw
ie g
eh
ört
halt
das,
fin
d i
ch s
chon
noch
, zu
r P
hys
ik d
azu
, d
ass
man
an
sich
ein
en
Verg
leic
h h
at
am
Sch
luss
zu
ein
em
Exp
eri
men
t. D
ass
man
nu
r w
en
nm
an
wir
kli
ch s
ich
au
f exp
eri
men
tell
e D
ate
n n
och
beru
fen
kan
n,
dan
n a
uch
tats
äch
lich
was
au
ssag
en
kan
n.
An
son
st i
st e
s sc
hon
wie
der
fast
nu
r M
ath
em
ati
k.
Wo m
an
irg
en
dw
elc
he K
on
zep
te a
ufs
tell
t u
nd
dan
n:
Ja,
die
Kon
zep
te s
ind
in
sic
hsc
hlü
ssig
un
d m
an
weiß
dan
n d
ie w
iders
pre
chen
sic
h n
ich
t, a
ber
man
weiß
üb
erh
au
pt
nic
ht
ob
sie
ein
en
Bezu
g z
u i
rgen
dw
as
hab
en
. U
nd
sola
ng
e d
as
Exp
eri
men
t eb
en
noch
irg
en
dw
ie d
ah
inte
rste
ht,
ist
es
eig
en
tlic
h k
lar
was
man
mach
t. M
an
gla
ub
t ein
fach
was
die
ses
Exp
eri
men
t fü
r K
on
seq
uen
zen
hat
un
d w
as
die
ses
Exp
eri
men
t all
es
zeig
en
kan
n.
Inso
fer
woll
te i
ch e
igen
tlic
h e
infa
ch
47
.
C Transcription of Interviews
122
weit
erh
in P
hys
ik m
ach
en
un
d n
ich
t M
ath
em
ati
k.
Rein
hard
Ok,
das
ist
der
Kern
. Vers
teh
e.
Du
sie
hst
sozu
sag
en
das
Exp
eri
men
t n
och
als
...?
48
.Jo
nas E
ine R
ech
tfert
igu
ng
fü
r d
ie T
heori
e.
49
.R
ein
hard
Oh
, ein
e R
ech
tfert
igu
ng
. G
ut.
Un
d d
as
hie
r n
och
mög
lich
.5
0.
Jon
as A
lso u
m d
as
ad
ab
surd
um
zu
tre
iben
bin
ich
mir
gar
nic
ht
so s
ich
er
ob
Str
ing
theori
e w
irkli
ch jetz
t P
hys
ik i
st.
Od
er
doch
nic
ht
eh
er
Meta
ph
ysik
.5
1.
Rein
hard
Das
wäre
die
Fra
ge g
ew
ese
n,
weil
du
au
ch s
chon
vorh
er
bei
der
All
gem
ein
en
[Rela
tivi
täts
theori
e]
gesa
gt
hast
: O
k,
das
geh
t sc
hon
ein
bis
sch
en
in
die
Ric
htu
ng
...
52
.
Jon
as D
ie A
llg
em
ein
e [
Rela
tivi
täts
theori
e]
kan
n m
an
noch
an
han
d v
on
Mess
un
gen
veri
fizi
ere
n.
Inso
fern
ist
es
da n
och
nic
ht
so a
bg
efa
hre
n w
ie b
ei
der
Str
ing
theori
e.
Ab
er
die
All
gem
ein
e [
Rela
tivi
täts
theori
e]
ist
ein
fach
nu
r w
eil
's e
inm
al
seh
rsc
hw
ieri
ge G
leic
hu
ng
en
sin
d.
Da k
an
n m
an
eig
en
tlic
h f
ast
nic
hts
an
aly
tisc
hm
ach
en
, so
nd
ern
mu
ss f
ast
all
es
nu
meri
sch
mach
en
. U
nd
das
hat
mic
h i
rgen
dw
ieein
bis
sch
en
ab
gesc
hre
ckt.
Das
ist
eig
en
tlic
h m
eh
r w
as
ich
mein
te.
Es
ist
ein
fach
zu s
chw
ieri
g u
m s
chn
ell
irg
en
dw
elc
he A
uss
ag
en
zu
mach
en
.
53
.
Rein
hard
Das
ist
hie
r ir
gen
dw
ie d
er
Vort
eil
, w
eil
er
Ap
para
t, a
lso d
er
theore
tisc
he A
pp
ara
tse
hr
gre
ifb
ar
ist.
54
.
Jon
as G
en
au
. A
lso a
n s
ich
fan
d i
ch Q
uan
ten
ein
fach
ein
fach
er.
55
.R
ein
hard
Sie
hst
du
neb
en
die
sem
Best
äti
gu
ng
swert
den
das
Exp
eri
men
t, w
ie d
u g
esa
gt
hast
, h
at,
noch
irg
en
dw
ie e
inen
an
dere
n Z
ug
an
g..
.? D
ass
es
irg
en
dw
ie b
eim
Vers
tän
dn
is h
ilft
. N
ich
t n
ur
in d
er
Th
eori
e z
u v
erw
eil
en
, so
nd
ern
das
Din
g a
uch
am
Arb
eit
en
, im
Exp
eri
men
t zu
bau
en
od
er
zu s
eh
en
.
56
.
Jon
as A
lso jetz
t w
irkli
ch d
iese
In
stru
men
te z
u s
eh
en
un
d i
rgen
dw
elc
he A
uss
chlä
ge a
nM
ess
ap
para
ten
hat
mir
bis
her
nic
hts
geb
rach
t. W
eil
ich
da n
ich
t g
en
ug
vers
teh
e.
Ab
er
wen
n m
an
sic
h e
ben
mit
den
exp
eri
men
tale
n P
hys
ikern
un
terh
ält
, d
an
nm
erk
t m
an
, d
ass
die
irg
en
dw
ie e
inen
an
dere
n B
ezu
g h
ab
en
. W
eil
bei
den
en
ist
halt
jetz
t d
iese
s K
on
zep
t, i
st jetz
t n
ich
t ein
e F
orm
el,
son
dern
es
ist
der
Au
ssch
lag
an
dem
In
stru
men
t, d
er
da u
nd
da p
ass
iert
. U
nd
das
ist
irg
en
dw
ie..
. D
as
ist
kom
isch
.A
m A
nfa
ng
red
et
man
an
ein
an
der
vorb
ei,
ab
er
es
ist
an
sic
h i
nte
ress
an
t. A
lso i
chg
lau
b,
dass
man
's d
ad
urc
h e
in b
issc
hen
bess
er
ken
nen
lern
t. W
ob
ei
bis
her
ärg
ere
ich
mic
h e
igen
tlic
h m
eh
r d
arü
ber.
57
.
Rein
hard
Dass
das
so u
nte
rsch
ied
lich
e K
on
zep
te s
ind
vom
Vers
teh
en
?5
8.
Jon
as D
as
sie n
ich
t ü
ber
irg
en
dw
elc
he G
leic
hu
ng
en
red
en
kön
nen
. W
eil
son
st k
an
n i
ch e
sn
ich
t ü
berp
rüfe
n.
Da m
uss
ich
dan
n s
ag
en
ja v
iell
eic
ht.
Kan
n s
ein
, d
ass
das
dam
itzu
tun
hat.
Ab
er
eig
en
tlic
h i
st e
s d
och
das
hie
r [k
lop
ft a
uf
den
Tis
ch].
Als
o m
an
vers
teh
t zu
min
dest
noch
ein
e a
nd
ere
Seit
e.
Lern
t si
e k
en
nen
, ic
h w
eiß
nic
ht
ob
man
sie
vers
teh
t. W
ah
rsch
ein
lich
sch
on
un
d s
om
it w
ah
rsch
ein
lich
bess
er.
59
.
Rein
hard
Dan
n i
st ja d
ie F
rag
e,
wie
sie
ht'
s b
eim
Vers
tän
dn
is a
us?
Od
er,
wen
n d
u d
ir d
iese
Din
ge a
nsc
hau
st,
jetz
t Q
uan
ten
info
rmati
on
usw
., d
ie P
hän
om
en
e o
der
Eff
ekte
, w
ie6
0.
imm
er
man
das
nen
nen
soll
, w
ie i
st d
a d
ein
Vers
tän
dn
is?
Es
gib
t ja
die
Au
ssag
e,
dass
das
irg
en
dw
ie k
on
train
tuit
iv i
st u
nd
dass
das
nic
ht
mit
ein
er
täg
lich
en
ph
ysik
ali
sch
en
Beob
ach
tun
g v
ere
inb
ar
ist.
Un
d d
ass
das
irg
en
dw
ie p
rob
lem
ati
sch
ist
un
d b
efr
ied
igt
werd
en
soll
te.
Das
es
bess
er
pass
t.Jo
nas O
k.
Äh
mm
m.
Als
o ja.
Ich
mein
e m
an
sie
ht.
.. M
an
ist
ein
fach
gew
oh
nt
irg
en
dw
ieau
s d
er
Intu
itio
n,
dass
wen
n i
rgen
dein
ein
Körp
er
irg
en
dein
e E
igen
sch
aft
hat,
dass
dan
n d
ie E
igen
sch
aft
tats
äch
lich
da i
st.
Od
er,
dass
das
irg
en
dw
ie t
ats
äch
lich
reali
siert
ist
. In
der
Qu
an
ten
mech
an
ik m
uss
man
sic
h d
a v
oll
kom
men
von
vera
bsc
hie
den
. S
on
dern
, d
ass
sic
h v
iele
Eig
en
sch
aft
en
sic
h w
irkli
ch e
rst
fest
leg
en
,so
bald
man
eb
en
da e
ine M
ess
un
g m
ach
t. U
nd
sie
vorh
er
au
ch t
ats
äch
lich
nic
ht
fest
lieg
en
. U
nd
dass
es
irg
en
dw
ie s
ow
as
wie
Sta
nd
pu
nkts
ab
hän
gig
keit
gib
t. F
ür
ein
en
kan
n's
an
dere
s se
in,
als
fü
r ein
en
an
dere
n.
Als
o e
s si
nd
Ph
än
om
en
e d
iekon
teri
ntu
itiv
sin
d.
Die
man
sic
h i
rgen
dw
ie,
na ja,
vors
tell
en
kan
n?
Man
kan
n s
ich
maxi
mal
dara
n g
ew
öh
nen
.
61
.
Rein
hard
Die
Fra
ge i
st,
ob
man
sag
t, d
ass
... Je
tzt
hab
e i
ch m
ein
e q
uan
ten
mech
an
isch
eT
heori
e,
da r
ech
ne i
ch,
un
d d
a g
elt
en
sozu
sag
en
die
se D
ing
e..
.6
2.
Jon
as Ja
. A
n s
ich
ist
das
das
Op
tim
um
; d
as
stim
mt.
Ab
er
man
en
twic
kelt
sch
on
au
tom
ati
sch
, all
ein
e a
us
den
Gle
ich
un
gen
rau
s, i
rgen
dw
ie s
o e
in G
efü
hl.
Das
Gefü
hl
pass
t n
ich
t zu
dem
, w
as
man
vie
lleic
ht,
als
jetz
t ein
er
der
sich
dam
it n
ich
tb
esc
häft
igt
hat,
erw
art
en
wü
rde.
Ab
er
es
ist
trotz
dem
...
Irg
en
diw
e e
in G
efü
hl
ist
dan
n s
chon
da.
Als
o w
ah
rsch
ein
lich
ist
das
am
eh
est
en
was
dan
n a
ls I
ntu
itio
nb
eze
ich
net
werd
en
kan
n.
63
.
Rein
hard
Als
o w
en
n m
an
so e
inen
Um
gan
g h
at
mit
den
Din
gen
, d
ass
man
dan
n e
ine g
ew
isse
Selb
stve
rstä
nd
lich
keit
bekom
mt.
Wah
rsch
ein
lich
merk
t m
an
das
beim
Sp
rech
en
,w
en
n m
an
ein
fach
Vokab
eln
un
d g
ew
isse
Sätz
e s
ag
t, d
ie f
ür
an
dere
rech
tkon
train
tuit
iv w
äre
n.
Od
er
rech
t m
erk
wü
rdig
kli
ng
en
wü
rden
, w
en
n m
an
die
in
an
dere
n Z
usa
mm
en
hän
gen
sag
t.
64
.
Jon
as D
as
Pro
ble
m i
rgen
dw
ie,
wen
n m
an
...
Ne,
ich
weiß
jetz
t n
ich
t w
ie i
ch d
as
zusa
mm
en
fass
en
kan
n.
Ste
ll e
infa
ch n
och
mal
gan
z ku
rz d
ie F
rag
e.
Sorr
y.6
5.
Rein
hard
Äh
m.
Wir
ware
n g
era
de e
igen
tlic
h b
ei
der
Fra
ge,
ob
man
sic
h s
ozu
sag
en
an
die
seD
ing
e g
ew
öh
nen
kan
n.
Die
ses
Kon
train
tuit
ive d
as
man
sag
t, d
ass
es
viell
eic
ht
mög
lich
erw
eis
e v
ers
chw
ind
et
in d
em
man
sic
h m
it d
en
Din
gen
besc
häft
igt.
66
.
Jon
as Ja
. D
as
wü
rde i
ch a
uf
jed
en
Fall
sag
en
, d
ass
das
pass
iert
. Ic
h m
ein
e jetz
t is
t es
für
mic
h r
ela
tiv
selb
stve
rstä
nd
lich
, d
ass
wen
n i
ch ü
ber
ein
Beis
pie
l re
de,
dass
ich
dan
n w
eiß
: W
en
n jetz
t d
er
Beob
ach
ter
das
un
d d
as
mach
t, v
erä
nd
ert
sic
h d
as
Sys
tem
so u
nd
so,
un
d f
ür
an
dere
so.
67
.
Rein
hard
Als
o e
s is
t n
ich
t m
eh
r so
ein
e A
rt h
ypoth
eti
sch
e A
nn
ah
me,
die
man
im
mer
so i
mH
inte
rkop
f h
at
-- u
nte
r d
er
An
nah
me,
dass
dem
wir
kli
ch s
o i
st -
-, s
on
dern
es
ist
ein
fach
so.
68
.
Jon
as D
ie Q
uan
ten
mech
an
ik,
bzw
. d
as
Kon
zep
t, w
as
man
sic
h d
a a
ufg
eb
au
t h
at,
das
üb
ern
imm
t m
an
dan
n s
chon
. E
s is
t ein
fach
die
best
e B
esc
hre
ibu
ng
der
Welt
die
wir
bis
her
hab
en
un
d i
nso
fern
wen
det
man
das
dan
n w
irkli
ch a
uf
bre
itere
n E
ben
en
an
, als
es
viell
eic
ht
ged
ach
t is
t.
69
.
123
Inte
rpre
tati
on
en
/ T
heori
e /
Exp
eri
men
t
Rein
hard
Un
d d
ie F
rag
e,
wen
n m
an
das
jetz
t so
sag
en
wil
l, w
eil
es
ja I
nte
rpre
tati
on
en
der
Qu
an
ten
mech
an
ik g
ibt,
die
vers
uch
en
das
Vers
tän
dn
is i
rgen
dw
ie a
ufz
ulö
sen
. O
der
die
s zu
min
dest
irg
en
dw
ie m
it e
iner
Gesc
hic
hte
zu
verb
ind
en
, so
dass
es
irg
en
dw
ieb
ess
er
vers
tän
dli
ch i
st.
Un
d d
ie s
teh
en
ja s
ozu
sag
en
neb
en
ein
an
der.
In
wie
weit
sin
d d
ie f
ür
dic
h i
rgen
dw
ie r
ele
van
t, h
elf
en
dein
em
Vers
tän
dn
is,
od
er
sin
d d
ie..
.h
ab
en
kein
e A
uss
ag
ekra
ft s
ozu
sag
en
.
70
.
Jon
as N
a ja.
Es
ist
halt
was
worü
ber
man
nach
den
kt
bei
irg
en
dw
ie e
iner
Fla
sch
e W
ein
am
Ab
en
d o
der
so w
as.
In
sofe
r d
rau
e i
ch i
hn
en
mal
nic
ht
sovi
el
Au
ssag
ekra
ft z
u,
weil
es
sin
d e
infa
ch..
. N
a ja,
es
gib
t ein
fach
die
Besc
hre
ibu
ng
en
. U
m e
s kon
kre
ter
zu m
ach
en
: M
an
kön
nte
sag
en
, ja
un
ser
gesa
mte
s W
elt
all
befi
nd
et
sich
in
ein
em
fest
em
Zu
stan
d.
In e
inem
Zeig
er
oh
ne..
. L
etz
en
dli
ch g
ibt
es
dam
it d
och
wie
der
Dete
rmin
ism
us.
71
.
Rein
hard
Ein
en
voll
stän
dig
en
.7
2.
Jon
as E
ben
ein
voll
stän
dig
er.
Sob
ald
ich
all
erd
ing
s n
ur
ein
Teil
syst
em
betr
ach
te v
erl
iere
ich
eb
en
wie
der
die
sen
Dete
rmin
ism
us
un
d m
uss
mic
h d
an
n m
it p
rob
ab
ilis
tisc
hen
Au
ssag
en
zu
frie
den
geb
en
. Ja
, d
as
gib
t es
zum
Beis
pie
l. M
an
kan
n ü
berl
eg
en
jetz
t,w
äre
es
sch
lüss
ig m
it d
em
was
wir
bis
her
wis
sen
. S
o w
eit
ich
weiß
gib
t's
da a
uch
nie
man
den
der
irg
en
dw
as
dag
eg
en
gesa
gt
hat.
Un
d..
. ja
...
ab
er.
.. L
etz
ten
dli
chsa
gen
kan
n m
an
's n
ich
t. E
s g
ibt
gen
au
so d
an
n d
iese
, d
iese
...
Ne d
as
mü
sste
...
Jad
as
mü
sste
eig
en
tlic
h d
an
n..
. Is
t es
dan
n d
ie..
. N
e d
as
ist
nic
ht
die
Vie
le-W
elt
en
.Ic
h m
ein
e e
s g
ibt
gen
au
so d
iese
Vie
le-W
elt
en
In
terp
reta
tion
. D
as
sich
bei
jed
er
En
tsch
eid
un
g e
ben
irg
en
wie
was
Neu
es
ab
-bra
nch
ed
. Ja
, g
en
au
au
f d
em
gle
ich
en
Gra
d.
73
.
Rein
hard
Ab
er
zum
ind
est
....
74
.Jo
nas Sie
sin
d e
ben
da,
man
üb
erl
eg
t's
sich
. M
an
sp
ielt
dam
it r
um
: W
ürd
e d
as
den
ng
eh
en
? O
der
was
kön
nte
das
den
n b
ed
eu
ten
? A
ber
letz
ten
dli
ch,
wen
n m
an
dan
nin
s L
ab
or
geh
t od
er
so w
as,
dan
n n
imm
t m
an
doch
wie
der
irg
en
dw
ie n
ur
ein
fach
den
Form
ali
smu
s, d
en
man
hat
oh
ne jetz
t d
a e
ine I
nte
rpre
tati
on
dem
un
bed
ing
tg
eb
en
zu
mü
ssen
.
75
.
Rein
hard
Vers
teh
e.
Ab
er
sozu
sag
en
die
Dis
ku
ssio
n b
est
eh
t n
och
.7
6.
Jon
as E
s is
t in
tere
ssan
t. I
nte
ress
an
t si
ch z
u ü
berl
eg
en
ob
da..
. w
irkli
ch o
b's
dan
n t
ote
Katz
e u
nd
ein
e l
eb
en
dig
e K
atz
e g
ibt.
Od
er
ob
es
jetz
t vo
n A
nfa
ng
an
kla
r is
t, jetz
tis
t d
ie K
atz
e t
ot
od
er
so.
77
.
Rein
hard
Wü
rdest
du
seh
en
, d
ass
gera
de d
ie A
rbeit
die
gem
ach
t w
ird
eig
en
tlic
h f
ast
dara
uf
ab
zielt
da z
u s
ag
en
...
die
Fra
ge z
u b
ean
twort
en
. A
lso w
en
n z
u s
ag
st,
Sch
röd
ing
ers
Katz
e,
dass
zu
m B
eis
pie
l je
tzt
wen
n i
ch d
ie o
pto
-mech
an
isch
en
Din
ger
hern
eh
me,
die
sch
on
ein
bis
serl
makro
skop
isch
er
sin
d,
sch
on
in
die
Ric
htu
ng
geh
en
wü
rden
.
78
.
Jon
as Ic
h g
lau
be n
ich
t, d
ass
man
es
voll
stän
dig
besc
hre
iben
kan
n. A
lso,
dass
man
dah
inkom
mt.
79
.
Rein
hard
Als
o,
dass
es
sozu
sag
en
ein
Test
kri
teri
um
gib
t, w
o m
an
dan
n s
ag
t: O
k,
das
ist
nu
rm
it d
iese
r ein
en
In
terp
reta
tion
kom
pati
bel
un
d d
esw
eg
en
ist
die
die
Ric
hti
ge.
80
.
Jon
as K
an
n i
ch m
ir n
ich
t vo
rste
llen
. A
lso i
ch g
lau
be,
dass
man
all
e I
nte
rpre
tati
on
en
irg
en
dw
ie d
an
n n
och
zu
rech
t fl
icken
kan
n u
m d
an
n d
as
noch
zu
erk
läre
n.
Wah
rsch
ein
lich
sch
eid
en
ein
paar
au
s, a
ber
ich
gla
ub
e n
ich
t, d
ass
man
sic
hw
irkli
ch e
nts
cheid
en
kan
n a
m S
chlu
ß.
Ah
, [l
ach
t] 1
90
0 w
are
n w
ir w
eit
er,
[Lach
en
]w
as
das
an
geh
t.
81
.
Rein
hard
Als
o i
n d
em
Sin
ne i
st e
s kein
Pro
ble
m,
dass
es
da s
o e
ine V
ielf
alt
an
Inte
rpre
tati
on
en
gib
t, d
ie i
m H
inte
rgru
nd
...
82
.
Jon
as Ic
h g
lau
be m
an
hat
sich
irg
en
dw
ie s
o e
in b
issc
hen
davo
n v
era
bsc
hie
det,
dass
man
...
Als
o z
um
ind
est
ich
hab
e m
ich
fü
r m
ich
davo
n v
era
bsc
hie
det,
dass
ich
wir
kli
ch e
xakt
besc
hre
iben
kan
n w
ie d
ie W
elt
fu
nkti
on
iert
. Ic
h k
an
n n
ur
ein
fach
das
Mod
ell
neh
men
un
d i
n d
em
Mod
ell
kan
n i
ch's
besc
hre
iben
, u
nd
dan
n m
uss
ich
mic
h d
am
it...
Mu
ss i
ch i
mm
er
im H
inte
rkop
f eig
en
tlic
h h
ab
en
: D
as
kan
n a
uch
all
es
fals
ch s
ein
, ir
gen
dw
ie.
Ab
er
bis
her
hab
en
...
sag
en
all
e T
est
s d
ie w
ir g
em
ach
th
ab
en
, es
pass
t w
ah
rsch
ein
lich
.
83
.
Rein
hard
Das
wü
rde a
uch
den
Bezu
g z
um
Exp
eri
men
t erk
läre
n.
Dass
man
das
Mod
ell
im
mer
noch
ab
gle
ich
en
mu
ss g
eg
en
das
[Exp
eri
men
t],
dam
it m
an
halb
weg
s ein
e r
ich
tig
eA
uss
ag
e t
riff
t.
84
.
Jon
as G
en
au
. Ja
.8
5.
Tech
nis
ch
er
Fort
sch
ritt
Rein
hard
Vers
teh
e.
Wie
wü
rdest
du
eig
en
tlic
h jetz
t d
en
tech
nis
chen
Wan
del.
.. D
ieM
ög
lich
keit
en
die
geg
eb
en
sin
d a
uf
tech
nis
cher
Seit
e,.
..8
6.
Jon
as W
ie s
ich
der
en
twic
kelt
hat,
od
er?
87
.R
ein
hard
Ja,
das
es
sich
en
twic
kelt
hat.
Als
o d
as
die
se D
ing
e s
ozu
sag
en
jetz
t m
ög
lich
sin
d.
Die
Qu
an
ten
mech
an
ik i
st a
lt.
88
.
Jon
as Ä
h,
ist
sie s
chon
?[la
cht]
Was
wü
rde i
ch d
azu
sag
en
? A
lso d
ie M
ög
lich
keit
en
sin
d d
aau
f je
den
Fall
deu
tlic
h b
ess
er
gew
ord
en
. W
en
n m
an
sic
h a
llein
e..
. Ic
h w
eiß
nic
ht
ob
das
so g
an
z in
den
An
fän
gen
war,
ab
er
wen
n m
an
sic
h d
en
Ste
rn-G
erl
ach
Vers
uch
[1
92
2,
Beob
ach
tun
g d
er
Ric
htu
ng
squ
an
telu
ng
von
Dre
him
pu
lsen
(=
Sp
in)
von
Ato
men
] an
sch
au
t, d
en
Ste
rn u
nd
Gerl
ach
gem
ach
t h
ab
en
. D
a h
ab
en
die
so
ein
e g
roß
en
Au
fwan
d b
etr
eib
en
mü
ssen
, u
m e
ine A
ufw
eit
un
g v
on
so e
iner
Ell
ipse
zu s
eh
en
, w
o m
an
am
Sch
luß
dan
n n
ich
t m
al
sag
en
kon
nte
: Ja
, d
as
hat
sich
wir
kli
ch g
esp
alt
en
. S
on
dern
da i
st b
loß
da e
in b
issc
hen
meh
r, d
a e
in b
issc
hen
meh
r u
nd
da e
in b
issc
hen
meh
r, u
nd
in
der
Mit
te h
alt
ein
bis
sch
en
wen
iger.
Un
dd
ara
us
hab
en
sie
dan
n w
as
gesc
hlu
ßfo
lgert
.
89
.
Wen
n m
an
jetz
t h
eu
te d
as.
.. A
lso g
ut,
wir
hab
en
das
im F
ort
gesc
hri
tten
en
-P
rakti
ku
m i
n s
o e
in,
zwei,
dre
i S
tun
den
noch
mal
nach
gem
ach
t, d
iese
n V
ers
uch
.U
nd
wir
seh
en
ein
fach
ein
e..
. ein
fach
zw
ei
Lin
ien
un
d v
iell
eic
ht
noch
so e
inb
issc
hen
Rau
sch
en
in
der
Mit
te.
Da i
st e
s au
f je
den
Fall
deu
tlic
h e
infa
cher
gew
ord
en
dan
n z
u s
ag
en
, ja
die
Th
eori
e s
tim
mt.
Bei
den
en
mu
sste
man
sic
h d
an
n
90
.
C Transcription of Interviews
124
sch
on
rech
tfert
igen
: ja
es
ist
seh
r w
ah
rsch
ein
lich
, d
ass
es
rich
tig
ist
, so
nst
kön
nte
n w
ir u
ns
jetz
t d
iese
kom
isch
en
Ab
weic
hu
ng
en
nic
ht
wir
kli
ch e
rklä
ren
. E
sis
t au
f je
den
Fall
ein
fach
er
gew
ord
en
, d
a s
o A
uss
ag
en
zu
tre
ffen
un
d a
uch
irg
en
dw
ie d
eu
tlic
h f
ein
ere
Üb
erp
rüfu
ng
en
pra
kti
sch
zu
hab
en
, vo
n d
er
Th
eori
e.
Od
er
die
se g
an
zen
Fü
r u
nd
Wid
er
für
das
Mic
hels
on
s-In
terf
ero
mete
r[U
nte
rsu
chu
ng
des
Lic
htä
thers
als
Med
ium
fü
r d
ie A
usb
reit
un
g d
es
Lic
hts
]. W
om
an
che a
m A
nfa
ng
gesa
gt
hab
en
, d
ass
: Ja
, oh
. Je
tzt
dre
hen
wir
das
in e
ine a
nd
ere
Ric
htu
ng
un
d w
ir k
rieg
en
gen
au
das
Gle
ich
e r
au
s. U
nd
dan
n k
om
mt
späte
r w
ied
er
ein
er:
Ja i
hr
hab
t d
as
üb
erh
au
pt
nic
ht
gekon
nt.
Ih
r h
ab
t vi
el
zu v
iele
Ab
weic
hu
ng
en
um
wir
kli
ch s
ag
en
zu
kön
nen
, d
ass
ih
r d
as
tats
äch
lich
jetz
tg
em
ess
en
hab
t. V
iell
eic
ht
gib
t's
ja d
och
noch
den
Äth
er.
Das
ist
üb
erh
au
pt
nic
ht
kla
r. U
nd
dan
n m
ach
t m
an
das
halt
wie
der
gen
au
er
mit
neu
en
In
stru
men
ten
, u
nd
wie
der
gen
au
er
mit
neu
en
In
stru
men
ten
un
d i
rgen
dw
an
n k
an
n d
an
n a
uch
kein
er
meh
r w
as
dag
eg
en
sag
en
.
91
.
Rein
hard
Als
o e
s is
t sc
hon
kein
sch
lech
tes
Ind
iz,
dass
es
da S
tud
en
ten
- od
er
Sch
üle
rexp
eri
men
te g
ibt,
die
das
nach
weis
en
...
92
.
Jon
as G
en
au
. D
ie e
infa
ch d
as
ab
deck
en
kön
nen
, w
as
in d
en
zw
an
zig
er
Jah
ren
od
er
au
chso
gar
sch
on
vie
rzig
er
Jah
ren
irg
en
dw
elc
he L
eu
te m
it s
eh
r, s
eh
r vi
el
Au
fwan
d..
. D
iew
irkli
ch d
a M
illi
on
en
rein
gest
eck
t h
ab
en
, od
er
was
weiß
ich
wie
viel
Geld
man
da
jew
eil
s za
hle
n m
uss
te,
dan
n jetz
t fü
r so
Stu
den
ten
nach
gem
ach
t w
erd
en
kan
n.
Das
zeig
t au
f je
den
Fall
au
f, d
ass
es
sich
an
sch
ein
en
d v
erb
ess
ert
hat.
Das
man
jetz
tir
gen
dw
elc
he M
illi
on
en
rein
steck
t, d
ass
man
dan
n g
an
z sc
hön
vie
l b
ess
ere
Erg
eb
nis
se r
au
skri
eg
t, o
der
fein
ere
Erg
eb
nis
se.
93
.
Rein
hard
Ja,
bzw
. es
sch
ein
t au
ch..
. M
an
sch
ein
t d
ie A
nw
en
du
ng
smög
lich
keit
en
en
tdeck
t zu
hab
en
un
d d
esw
eg
en
sch
ein
t so
zusa
gen
meh
r D
ruck
dah
inte
r zu
sein
. D
as
ist
die
Fra
ge?
Ab
er
sch
ein
t zu
min
dest
en
s so
.
94
.
Jon
as Ic
h d
en
ke m
al
die
Gese
llsc
haft
hat
inzw
isch
en
ein
fach
fest
gest
ell
t, d
ass
da d
och
wie
der
imm
er
irg
en
dw
as,
was
ab
fäll
t, w
as
man
verw
ert
en
kan
n.
Wen
n m
an
sic
hsc
hon
sovi
el
au
f d
ie E
ntw
icklu
ng
beru
ft,
das
mach
t n
atü
rlic
h s
chon
ein
bis
sch
en
meh
r D
ruck
. E
s si
nd
au
ch jetz
t ein
fach
deu
tlic
h m
eh
r L
eu
te,
die
sic
h u
m s
ow
as
wie
ein
en
Fort
sch
ritt
kü
mm
ern
; als
es
dam
als
war.
95
.
Rein
hard
[leis
e]
Das
hab
e i
ch s
chon
gefr
ag
t.9
6.
Pers
pekti
ve
Rein
hard
Wie
sie
ht
es
eig
en
tlic
h P
lan
-mäß
ig b
ei
dir
au
s?9
7.
Jon
as D
an
ach
?9
8.
Rein
hard
Ja,
dan
ach
.9
9.
Jon
as Ja
, ic
h w
ürd
e g
ern
e e
inen
Dokto
r m
ach
en
. W
o w
eiß
ich
nic
ht.
Wah
rsch
ein
lich
gan
zg
ern
e w
eit
er
Qu
an
ten
op
tik,
od
er
Op
to-M
ech
an
ik,
od
er
Qu
an
ten
info
rmati
on
.Ir
gen
dw
ie s
o i
n d
em
bre
iten
Feld
. Ja
, m
al
sch
au
en
. W
as
da g
en
au
weiß
ich
ab
er
noch
nic
ht.
Als
o i
ch h
ab
nic
hts
wir
kli
ch i
n A
uss
ich
t.
10
0.
Rein
hard
Die
Dip
lom
arb
eit
ein
mal
als
Nah
ziel?
10
1.
Jon
as D
ie D
iplo
marb
eit
ein
mal
nach
Hau
se f
ah
ren
. B
ish
er
kam
's m
ir a
uch
so v
or
wie
wen
n e
igen
tlic
h s
ich
die
Pro
fs,
Jen
s E
isert
od
er
so w
as
zum
Beis
pie
l, s
ich
da s
chon
irg
en
dw
ie d
aru
m k
üm
mert
un
d m
ir d
an
n s
ag
en
: B
ew
erb
dic
h m
al
bei
dem
un
dd
em
, d
as
wü
rde e
igen
tlic
h r
ela
tiv
gu
t p
ass
en
. D
a k
an
nst
du
das
un
d d
as
mach
en
.
10
2.
Rein
hard
Als
o d
ie t
reib
en
das
sch
on
in
ein
e R
ich
tun
g,
dass
da L
eu
te e
nts
teh
en
die
das
mach
en
.1
03
.
Jon
as D
ie h
ab
en
da i
rgen
dw
ie s
chon
ein
bis
sch
en
ein
en
Üb
erb
lick
, sc
hein
t es
mir
.1
04
.R
ein
hard
Es
sch
ein
t d
a s
ozu
sag
en
, zu
min
dest
en
s h
ier
im A
ufb
au
beg
riff
en
zu
sein
. D
azu
min
dest
en
s D
ing
e i
n d
ie R
ich
tun
g v
ora
nzu
bri
ng
en
.1
05
.
Jon
as G
en
au
, es
irg
en
dw
ie i
mm
er
noch
so,
dass
irg
en
dw
ie a
lles
wo "
Qu
" d
rin
ste
ckt,
ist
ein
fach
gera
de i
n.
Da h
at
man
au
ch g
ute
Mög
lich
keit
en
selb
st n
och
was
zum
ach
en
[la
cht]
.
10
6.
Rein
hard
Vers
teh
e.
10
7.
Jon
as Je
meh
r "Q
u"s
dest
o b
ess
er.
10
8.
Vers
ch
rän
ku
ng
Rein
hard
Im P
rin
zip
wäre
n d
as
mein
e F
rag
en
gew
ese
n.
Wen
n d
u n
ich
ts..
.1
09
.Jo
nas Je
tzt
hab
en
wir
nic
ht
viel
zur
Vers
chrä
nku
ng
gem
ach
t? I
ch w
eiß
nic
ht,
jetz
t d
air
gen
dw
as
au
s d
em
Näh
kast
en
was
darü
ber
zu s
ag
en
ist
natü
rlic
h a
uch
nic
ht
un
bed
ing
t ein
fach
. A
n s
ich
was
Vers
chrä
nku
ng
ist
, d
efi
nie
rt s
ich
bei
mir
hau
pts
äch
lich
eig
en
tlic
h d
am
it w
as
man
halt
mach
en
kan
n.
Weil
irg
en
wie
was
es
ist,
gla
ub
e i
ch w
eiß
kein
er
so r
ich
tig
. M
an
weiß
in
zwis
chen
so e
in b
issc
hen
wie
man
es
qu
an
tifi
ziert
. W
ie m
an
sag
en
kan
n i
ch h
ab
e v
iel,
ich
hab
e w
en
igVers
chrä
nku
ng
. U
nd
man
...
Na ja,
was
man
dan
n e
ben
fü
r E
ffekte
seh
en
wü
rde.
Irg
en
dw
ie T
ele
port
ati
on
od
er
Info
rmati
on
süb
ert
rag
un
g.
Gen
au
. E
infa
ch n
ur
irg
en
dw
ie a
ls e
ine R
ess
ou
rce.
11
0.
Rein
hard
Un
d w
ürd
est
du
seh
en
, d
ass
man
dara
us
meh
r E
rken
ntn
is g
ew
inn
t. W
en
n jetz
tein
mal
die
Fra
ge..
.1
11
.
Jon
as A
lso A
nw
en
du
ng
au
f je
den
Fall
. A
lso i
ch m
ein
e d
ie A
nw
en
du
ng
en
die
bis
her
au
sd
en
Qu
an
ten
rau
sgekom
men
sin
d,
beru
fen
sic
h f
ast
--
nein
das
kan
n i
ch jetz
t n
ich
tsa
gen
--.
.. A
ber
es
gib
t au
f je
den
Fall
An
wen
du
ng
en
wie
in
der
Kry
pto
gra
ph
ie,
eb
en
zum
Beis
pie
l, o
der
jetz
t eb
en
in
der
Kon
troll
e v
on
irg
en
dw
elc
hen
kle
inen
Sys
tem
en
. U
nd
da s
pie
lt d
an
n s
chon
die
Vers
chrä
nku
ng
eb
en
ein
e p
rin
zip
iell
eR
oll
e.
Als
o z
um
al
wir
jetz
t au
ch..
. Z
um
al
irg
en
dw
ie i
nzw
isch
en
mein
Vers
tän
dn
isis
t, d
ass
Vers
chrä
nku
ng
eig
en
tlic
h d
as
ist,
was
die
Qu
an
ten
info
rmati
on
...
Od
er
was
die
Qu
an
ten
info
rmati
on
üb
erh
au
pt
erm
ög
lich
t, d
ass
die
irg
en
dw
ie b
ess
er
wü
rde
als
die
Kla
ssic
he.
Dass
man
dam
it S
ach
en
mach
en
kan
n,
die
die
Kla
ssis
che n
ich
tkan
n.
Das
ist
au
f je
den
Fall
au
f d
ie V
ers
chrä
nku
ng
zu
rück
zufü
hre
n.
Inso
fern
, ja
.A
ber
was
es
ist,
weiß
man
au
ch n
ich
t so
ric
hti
g,
wü
rde i
ch jetz
t b
eh
au
pte
n.
Als
o
11
2.
125
man
che h
ab
en
wah
rsch
ein
lich
ein
bess
ere
s G
efü
hl,
man
che e
in s
chle
chte
res
Gefü
hl.
Ich
hab
e n
och
kein
so r
ich
tig
es.
Rein
hard
Als
o d
u b
len
dest
...
Eig
en
tlic
h n
ich
t ein
mal
au
sble
nd
en
wah
rsch
ein
lich
, so
nd
ern
es
ist
halt
nic
ht
rele
van
t.1
13
.
Jon
as Ic
h e
infa
ch w
irkli
ch n
och
kein
Gefü
hl
dafü
r. D
azu
hab
e i
ch w
ah
rsch
ein
lich
zu
wen
ig m
itg
em
ach
t. I
ch w
eiß
wie
so e
ine T
ele
port
ati
on
mit
so V
ers
chrä
nku
ng
fun
kti
on
iert
. U
nd
ich
weiß
wie
ich
dam
it m
eh
r In
form
ati
on
üb
ert
rag
en
kan
n.
Un
dic
h w
eiß
au
ch w
ie i
ch V
ers
chrä
nku
ng
eb
en
mess
en
kan
n,
od
er
qu
an
tifi
ziere
n k
an
n.
Un
d a
n s
ich
ist
das
für
mic
h d
an
n V
ers
chrä
nku
ng
. D
iese
r op
era
tion
ell
e K
om
ple
x.D
am
it k
an
n i
ch a
ber
au
ch n
ich
t w
irkli
ch s
ag
en
, w
as
es
jetz
t...
11
4.
Rein
hard
Wie
wü
rdest
du
den
An
wen
du
ng
sbere
ich
der
Vers
chrä
nku
ng
seh
en
? E
s sc
hein
t ja
nic
ht
an
die
Grö
ßen
skala
geb
un
den
zu
sein
od
er
an
das
Sys
tem
. E
s sc
hein
t ja
meh
rso
, w
en
n m
an
das
sag
en
wil
l, p
rin
zip
iell
en
Ch
ara
kte
r zu
hab
en
. S
ob
ald
ich
ein
Sys
tem
en
tsp
rech
en
d p
räp
ari
ere
n k
an
n,
en
tsp
rech
en
d v
on
der
Um
welt
iso
liere
nkan
n,
hab
e i
ch d
ie M
ög
lich
keit
Vers
chrä
nku
ng
herz
ust
ell
en
.
11
5.
Jon
as G
en
au
. W
ob
ei
das
Isoli
ere
n e
ben
dan
n,
gera
de w
an
n e
s an
die
Grö
ße g
eh
t, d
er
zen
trale
Pu
nkt
des
Pro
ble
ms
ist.
Un
d s
o,
wori
n m
an
dan
n g
en
au
die
An
wen
du
ng
sieh
t?
11
6.
Rein
hard
Na ja,
die
Fra
ge i
st w
ie d
u s
ozu
sag
en
den
Sta
tus
sieh
st.
Weil
das
sch
ein
t ja
au
chein
e g
ew
isse
Merk
wü
rdig
keit
au
szu
mach
en
, d
as
es
syst
em
un
ab
hän
gig
ist
. O
der,
das
es
eh
er
ein
en
pri
nzi
pie
llen
Ch
ara
kte
r h
at.
11
7.
Jon
as A
lso w
ir h
ab
en
wir
kli
ch m
it d
em
Iso
liere
n i
st e
s d
as
grö
ßte
Pro
ble
m.
Un
dd
esw
eg
en
geh
t es
eb
en
mit
kle
inen
Sys
tem
en
wie
irg
en
dw
elc
hen
Ato
men
, od
er
hau
pts
äch
lich
natü
rlic
h L
ich
t, v
erd
am
mt
gu
t u
nd
all
es
darü
ber
hin
au
s w
ird
im
mer
ved
am
mt
sch
wie
rig
. U
nd
wen
n,
nu
r m
it g
roß
em
Au
fwan
d.
Da g
eh
t n
och
nic
ht
seh
rvi
el
An
wen
du
ng
wü
rde i
ch s
ag
en
. E
s is
t all
es
noch
pri
nzi
pie
ll u
nd
pro
of
of
con
cep
t.
11
8.
Rein
hard
Sola
ng
e k
ein
e A
nw
en
du
ng
da i
st,
od
er
nic
ht
so A
rt d
ie M
ög
lich
keit
da i
st,
das
irg
en
dw
ie w
irkli
ch s
o a
uch
in
grö
ßere
n S
kale
n z
u f
ass
en
, w
ürd
est
du
sag
en
, d
as
ist
nic
ht
gan
z si
cher,
dass
es
au
ch d
ort
rele
van
t se
in k
ön
nte
. Vers
teh
st d
u w
as
ich
mein
e?
Weil
die
Th
eori
e g
ibt
ja n
ich
t vo
r, d
ie G
röß
en
skala
, od
er
wo d
as
sein
eG
ren
zen
hat,
od
er
sein
e L
imit
ieru
ng
. A
lso d
ie V
ers
chrä
nku
ng
.
11
9.
Jon
as A
lso i
ch b
in s
chon
der
Mein
un
g,
dass
die
Vers
chrä
nku
ng
wir
kli
ch ü
bera
llp
rin
zip
iell
au
ftre
ten
kan
n.
Un
d a
uft
rete
n w
ird
. D
ass
ich
ab
er
nic
ht
weiß
ob
man
jem
als
irg
en
dein
e A
nw
en
du
ng
mit
gro
ßen
Sys
tem
en
mach
en
kan
n,
weil
es
ein
fach
vom
Au
fwan
d h
er
viel
zu k
om
pli
ziert
ist
. D
as
mein
te i
ch.
Ab
er
es
wir
d ü
bera
ll..
. B
inm
ir w
irkli
ch s
ich
er,
dass
das
Pri
nzi
p w
irkli
ch ü
bera
ll a
nzu
wen
den
ist
. V
iell
eic
ht
kön
nte
man
sog
ar
irg
en
dw
elc
he P
lan
ete
n m
itein
an
der
vers
chrä
nken
.[la
cht]
12
0.
Rein
hard
Vers
teh
e.
12
1.
Jon
as A
lso z
um
ind
est
...
Sow
eit
seh
e i
ch d
as
jetz
t, d
ass
es
in d
er
Th
eori
e,
sob
ald
ich
die
so b
esc
hre
iben
kan
n:
Als
irg
en
dw
ie z
wei
Sys
tem
e m
it i
rgen
dw
elc
hen
Zu
stän
den
,d
ass
ich
dan
n d
iese
Zu
stän
de a
uch
vers
chrä
nken
kan
n.
12
2.
Rein
hard
Als
o s
ola
ng
e d
as
Exp
eri
men
t n
ich
ts g
eg
en
teil
iges
beh
au
pte
t. W
en
n n
ich
tir
gen
dw
an
n a
uf
ein
mal
au
ftau
chen
wü
rde..
.1
23
.
Jon
as W
en
n d
as
dan
n w
irkli
ch a
uft
au
chen
wü
rde,
dan
n w
ürd
e d
as
wir
kli
ch h
eiß
en
: D
an
nis
t u
nse
re Q
uan
ten
mech
an
ik i
rgen
dw
ie f
als
ch.
Un
d d
avo
n g
eh
e i
ch jetz
t g
era
de
nic
ht
au
s.[l
ach
t] I
nso
fern
bin
ich
der
Mein
un
g:
Das
mü
sste
au
f all
en
...
Das
geh
t au
fall
en
Skale
n.
12
4.
Rein
hard
Ok.
12
5.
Jon
as A
ber
ja d
as
kan
n w
irkli
ch..
. S
ow
as
kan
n z
u e
inem
Test
fü
r Q
uan
ten
mech
an
ikau
sart
en
, ir
gen
dw
ie a
m S
chlu
ß.
Od
er
Qu
an
ten
gen
ere
ll.
12
6.
Rein
hard
Ab
er
eh
er
ers
t w
en
n P
rob
lem
e a
uft
au
chen
. E
s w
ürd
e e
s n
ich
t b
est
äti
gen
wen
nn
ich
ts p
ass
iert
, so
nd
ern
eh
er
wen
n P
rob
lem
e a
uft
rete
n u
nd
das
nic
ht
meh
rfu
nkti
on
iere
n w
ürd
e..
.
12
7.
Jon
as A
lso w
en
n m
an
das
irg
en
dw
an
n r
ich
tig
gu
t u
nte
r K
on
troll
e h
at
so e
in S
yste
m z
uis
oli
ere
n,
sod
ass
es
nic
ht
meh
r se
ine V
ers
chrä
nku
ng
in
die
Um
geb
un
g a
bg
ibt,
pra
kti
sch
. A
lso d
ekoh
eri
ert
. W
en
n m
an
da i
rgen
dw
ie m
al
was
pri
nzi
pie
ll g
efu
nd
en
hat,
dass
man
das
exa
kt
od
er
voll
stän
dig
irg
en
dw
ie i
soli
ere
n k
an
n u
nd
man
dan
nkein
e V
ers
chrä
nku
ng
hers
tell
en
kan
n,
dan
n i
st w
as
seh
r kap
utt
. D
a m
uss
man
wah
rsch
ein
lich
fast
neu
an
fan
gen
. A
ber
davo
n g
eh
e i
ch n
ich
t au
s. A
ber
kan
nn
atü
rlic
h p
ass
iere
n.
12
8.
En
de
Rein
hard
Gu
t. D
an
ke f
ür
das
Inte
rvie
w.
12
9.
Jon
as Ja
, kein
Pro
ble
m.
13
0.
(no s
peaker)
[sm
all
talk
]1
31
.
C Transcription of Interviews
126
Flo
rian
_110525
Inte
rvie
w m
it M
ag
. F
lori
an
Bla
ser
vom
25
.05
.20
11
Tra
nsc
rib
ed
by
yott
a,
vers
ion
1 o
f 1
10
52
7
An
fan
g,
pers
ön
lich
e D
ate
n,
Au
sbil
du
ng
Rein
hard
In t
he b
eg
inn
ing
it'
s ju
st s
om
e g
en
era
l q
uest
ion
s. H
ow
old
are
you
?1
.F
lori
an
I am
30
.2
.R
ein
hard
Th
at
took y
ou
a w
hil
e.
3.
Flo
rian
I st
op
ped
cou
nti
ng
five
years
ag
o.
4.
Rein
hard
Wh
at
is y
ou
r ed
uca
tion
al
back
gro
un
d?
I m
ean
wh
ere
did
you
stu
dy?
5.
Flo
rian
I st
ud
ied
ph
ysic
s in
Sw
itze
rlan
d,
in N
eu
chate
l. I
t w
as
a v
ery
sm
all
un
ivers
ity
that
was
not
reall
y sp
eci
ali
zed
in
qu
an
tum
in
form
ati
on
stu
ff.
Most
of
the q
uan
tum
stu
ffI
learn
ed
...
So I
did
have
qu
an
tum
mech
an
ics
in m
y co
urs
es,
bu
t q
uan
tum
info
rmati
on
was
not
very
str
on
g.
An
d w
e n
eve
r ta
lked
ab
ou
t en
tan
gle
men
t th
ere
.A
s yo
u s
tud
ied
in
Vie
nn
a,
I g
uess
it
is q
uit
e t
he o
pp
osi
te.
6.
Rein
hard
An
d w
hen
did
you
com
e h
ere
?7
.F
lori
an
I ca
me h
ere
to d
o m
y d
iplo
ma t
hesi
s. I
sta
rted
in
th
e g
rou
p o
f Z
eil
ing
er
[An
ton
Zeil
ing
er]
. A
nd
basi
call
y I
start
ed
to w
ork
on
th
e o
pto
-mech
an
ics
exp
eri
men
ts i
nth
e v
ery
beg
inn
ing
.
8.
Rein
hard
So t
his
was
two y
ears
ag
o?
9.
Flo
rian
20
05
, 2
00
6.
An
d t
hen
aft
er
my
dip
lom
a t
hesi
s I
wen
t on
work
ing
in
th
e i
nd
ust
ry.
An
d t
hen
cam
e b
ack
for
a P
hD
.1
0.
Rein
hard
Wh
at
was
you
r d
iplo
ma t
hesi
s ab
ou
t?1
1.
Flo
rian
I d
id s
imu
lati
on
s of
the m
ech
an
ical
syst
em
s w
e h
ave
. A
nd
als
o w
ork
ed
on
th
eexp
eri
men
ts t
hat
pro
du
ced
th
e fi
rst
cooli
ng
of
the m
oti
on
of
the c
an
tile
ver.
12
.
Rein
hard
Wh
at
did
you
do i
n t
he i
nd
ust
ry?
13
.F
lori
an
In t
he i
nd
ust
ry I
did
com
pu
ter
stu
ff.
So n
o p
hys
ics.
14
.R
ein
hard
Wh
en
did
you
get
to e
nta
ng
lem
en
t? W
as
it ju
st h
ere
in
Vie
nn
a,
or
som
ew
here
befo
re?
15
.
Flo
rian
I th
ink t
hat
was
the r
easo
n t
o c
om
e t
o V
ien
na.
Du
rin
g m
y st
ud
ies
I st
art
ed
, so
Ile
arn
ed
a b
it a
bou
t en
tan
gle
men
t, a
nd
sta
rted
to r
ead
on
my
ow
n t
wo b
ooks.
Books
ab
ou
t q
uan
tum
in
form
ati
on
. I
start
ed
read
ing
th
e N
iels
en
an
d C
hu
an
g b
ook
16
.
[com
pre
hen
sive
in
trod
uct
ion
to q
uan
tum
com
pu
tati
on
an
d i
nfo
rmati
on
]. I
got
qu
ite
inte
rest
ed
. A
nd
I s
tart
ed
to r
ead
th
e p
ap
ers
th
at
were
goin
g i
n t
his
dir
ect
ion
. S
o i
tw
as
the t
ime o
f th
e c
lust
er
com
pu
tin
g w
ith
th
e m
ult
i-p
hoto
n e
xperi
men
ts.
An
d I
read
ab
ou
t th
is a
nd
so o
k t
here
is
this
gro
up
in
Vie
nn
a.
Th
ey
seem
ed
to b
e g
ood
at
that
an
d I
tri
ed
to a
pp
ly t
here
.R
ein
hard
An
d i
t w
ork
ed
.1
7.
Flo
rian
An
d i
t w
ork
ed
. T
hey
were
cra
zy e
nou
gh
.1
8.
Rein
hard
So t
hat
was
the r
easo
n t
o c
om
e h
ere
an
d join
th
e g
rou
p. B
eco
me i
nvo
lved
in
th
is.
An
d w
hat
are
you
r am
bit
ion
s to
get
don
e h
ere
. I
mean
you
r P
hD
pro
bab
ly?
19
.
Flo
rian
Yeah
, so
I a
m P
hD
. I
am
work
ing
on
a p
roje
ct t
o d
o a
lso t
he k
ind
of
exp
eri
men
tsth
at
we d
id w
ith
th
e m
irro
rs,
wh
ich
are
sti
ll c
on
tin
uin
g,
bu
t w
ith
tra
pp
ed
nan
op
art
icle
s in
stead
.
20
.
Rein
hard
So y
ou
an
d N
ikola
i [N
ikola
i K
iese
l] a
re w
ork
ing
on
th
e s
am
e e
xperi
men
t?2
1.
Flo
rian
Exa
ctly
.2
2.
Rein
hard
So i
t is
ju
st y
ou
tw
o,
or?
23
.F
lori
an
Th
ere
is
thir
d g
uy
nam
ed
Uro
s [U
ros
Deli
c].
24
.S
o a
gain
. A
s in
my
dip
lom
a t
hesi
s, i
t is
most
ly c
lass
ical
ph
ysic
s. W
ith
som
e c
han
cew
e w
ill
reach
th
e g
rou
nd
sta
te.
Th
at
wil
l b
e m
y P
hD
th
en
.2
5.
Rein
hard
Ok.
So t
hat
is y
ou
r P
hD
top
ic t
o g
et
there
?2
6.
Flo
rian
To g
et
there
is
qu
ite a
ch
all
en
gin
g g
oal.
It
mig
ht
stil
l h
ap
pen
.2
7.
Rein
hard
At
wh
at
tim
e s
cale
? H
ow
lon
g w
ill
it t
ake y
ou
, yo
u t
hin
k?
28
.F
lori
an
So I
a P
hD
usu
all
y th
ree y
ears
. B
ut
thre
e p
lus
inte
rnall
y. A
nd
I d
id o
ne a
nd
a h
alf
year
up
to n
ow
.2
9.
Rein
hard
So y
ou
got
an
oth
er
on
e a
nd
a h
alf
to g
et
it d
on
e.
30
.
Au
fgab
e i
m E
xp
eri
men
t /
Roll
e i
n d
er
Gru
pp
e
Rein
hard
As
alr
ead
y sa
id y
ou
are
work
ing
wit
h N
ikola
i [N
ikola
i K
iese
l] a
nd
Uro
s [U
ros
Deli
c].
I ta
lked
wit
h N
ikola
i an
yway
how
far
you
got
in t
he e
xperi
men
t. A
nd
at
wh
ich
sta
te y
ou
are
.
31
.
Flo
rian
So w
e r
eall
y w
an
t to
see t
he p
roof
of
pri
nci
ple
rig
ht
now
.3
2.
Rein
hard
Is t
here
an
y st
ress
fro
m o
ther
gro
up
s? D
o y
ou
kn
ow
of
oth
er
gro
up
s th
at
are
...?
33
.F
lori
an
Defi
nit
ely
. W
e k
now
a f
ew
gro
up
s w
ho a
re f
or
sure
work
ing
in
th
e s
am
e d
irect
ion
.[?
?? a
sen
ten
ce I
cou
ld n
ot
get
???]
34
.
127
Rein
hard
So t
hey
are
on
th
e s
am
e l
eve
l?3
5.
Flo
rian
It d
ep
en
ds.
On
e g
rou
p i
s m
ore
ad
van
ced
. W
e d
on
't k
now
a l
ot
of
the o
ther
gro
up
s,b
eca
use
nob
od
y h
as
pu
bli
shed
an
yth
ing
. E
xcep
t on
e g
rou
p h
as
pu
bli
shed
alr
ead
yso
me p
ap
er,
wh
ere
th
ey
don
't r
eall
y w
ere
in
tere
sted
in
cooli
ng
. B
ut
they
had
atr
ap
pin
g a
nd
measu
red
th
e B
row
nia
n m
oti
on
[st
och
ast
ic r
an
dom
move
men
t of
part
icle
s su
spen
ded
in
a fl
uid
] of
the p
art
icle
. A
nd
wit
h t
his
th
ey
then
sh
ow
ed
feed
back
cooli
ng
. O
ur
gu
ess
is
that
they
con
tin
ue i
n t
he s
am
e d
irect
ion
.
36
.
Rein
hard
Wou
ld b
e l
og
ical
to g
o o
n f
rom
th
ere
.3
7.
Cou
ld y
ou
desc
rib
e w
hat
you
r h
an
ds
on
job
is
at
the e
xperi
men
t? I
mean
, N
ikola
ito
ld m
e t
hat
you
did
at
the m
om
en
t L
ab
Vie
w [
gra
ph
ical
pro
gra
mm
ing
en
viro
nm
en
tto
deve
lop
measu
rem
en
t, t
est
, an
d c
on
trol
syst
em
s].
38
.
Flo
rian
Yeah
, cu
rren
tly
I am
doin
g L
ab
Vie
w.
We b
asi
call
y n
eed
to p
lan
an
d d
iscu
ss h
ow
we
wan
t to
do i
t. T
hat
is s
om
eth
ing
we d
o q
uit
e a
lot
wit
h N
ikola
i. W
e t
ry t
o g
et
the
ideas
to g
et
rid
of
the n
ois
e.
An
d h
ave
th
e b
est
measu
rem
en
t p
oss
ible
. T
hen
th
ere
is t
he r
eall
y h
an
d o
n w
ork
of
ali
gn
ing
th
e o
pti
cs.
Sett
ing
up
th
e e
lect
ron
ics
for
makin
g t
he s
etu
p w
ork
. A
nd
ad
just
ing
ele
ctro
nic
s, o
pti
cs a
nd
...
Wh
en
it'
s in
th
eexp
eri
men
t an
d i
f w
e s
ee t
he s
ign
al.
Late
ly w
e h
ave
seen
th
e s
ign
al
in t
he w
ay
we
wan
ted
it
to a
pp
ear.
An
oth
er
part
of
the job
is
act
uall
y to
make b
ets
wit
h N
ikola
i.W
heth
er
this
wil
l w
ork
or
not.
Th
at
ad
ds
som
e f
un
to i
t.
39
.
Rein
hard
Th
at
dep
en
ds
on
how
oft
en
you
win
. O
r lo
se.
40
.F
lori
an
We a
nyw
ay
go f
or
a b
eer.
Th
e b
et
is a
way
to r
an
dom
ize w
ho p
ays
.4
1.
Rein
hard
If t
he r
esu
lt i
s ok,
it's
fin
e.
42
.F
lori
an
So c
urr
en
tly
we g
et
the s
ign
al.
We r
ou
gh
ly k
now
how
to d
o t
he m
easu
rem
en
t. W
eare
sti
ll p
roce
ssin
g t
he d
ata
to s
ee i
f w
e h
ave
th
e e
ffect
th
at
we w
an
t. A
nd
th
e n
ext
step
, w
hat
we d
o i
n p
ara
llel,
is
just
to p
rog
ram
. To h
ave
an
au
tom
ati
zati
on
of
the
exp
eri
men
t. N
ow
th
at
we k
now
th
at
it s
om
eh
ow
sh
ou
ld w
ork
.
43
.
Inte
rpre
tati
on
/ T
heori
e /
Exp
eri
men
t
Rein
hard
So h
ow
wou
ld y
ou
see t
he c
on
nect
ion
betw
een
th
e t
heory
an
d t
he e
xperi
men
tal
part
of
this
exp
eri
men
t?4
4.
Flo
rian
Here
I t
hin
k t
he t
heory
is
pre
tty
clear.
In
th
e s
en
se t
hat.
.. S
o i
t is
a d
iffere
nt
syst
em
to w
hic
h w
e a
pp
ly t
he t
heory
th
at
is a
lread
y kn
ow
n.
So t
here
is
stil
l a l
ot
of
back
an
d f
ort
h.
Th
e i
nte
rest
ing
th
eory
part
is
the l
imit
ati
on
s of
the s
yste
m a
nd
how
we c
an
im
pro
ve t
hat.
So h
ere
in
th
eory
we h
ave
a c
oll
ab
ora
te o
f th
is p
roje
ct.
We h
ave
a c
oll
ab
ora
tion
wit
h t
he p
ers
on
s w
ho a
ctu
all
y p
rop
ose
d t
he e
xperi
men
t.S
o w
e d
on
't d
o m
ost
of
the t
heory
. B
ut
to p
red
ict
som
eth
ing
, w
e h
ave
to d
o t
he l
ast
bit
of
theory
in
ap
ply
ing
th
e c
alc
ula
tion
s.
45
.
Rein
hard
So a
t le
ast
to c
om
pare
th
e r
esu
lts
wit
h s
om
e t
heory
. W
hat
you
exp
ect
ed
.4
6.
Flo
rian
Exa
ctly
.4
7.
Fasz
inati
on
an
der
Qu
an
ten
mech
an
ik
Rein
hard
Wh
at
in y
ou
r eye
s is
it
that
fasc
inate
s yo
u a
bou
t q
uan
tum
mech
an
ics?
Or
wh
y yo
ud
o t
his
?4
8.
Flo
rian
So t
he e
asy
an
swer
is e
nta
ng
lem
en
t, r
igh
t. T
he m
ost
pro
fou
nd
moti
vati
on
is
the
fact
th
at
we h
ave
a t
heory
th
at
is h
ard
to g
rasp
in
norm
al
term
s, o
r co
mm
on
day
exp
eri
en
ce.
It i
s h
ard
to b
rin
g t
hat
kn
ow
led
ges
to t
he q
uan
tum
worl
d.
Or
to m
ake
an
an
alo
gy
of
the q
uan
tum
worl
d u
sin
g d
ay-
to-d
ay
exp
eri
en
ce.
I th
ink t
hat'
s q
uit
e a
revo
luti
on
in
sci
en
ce.
It d
idn
't s
tart
rece
ntl
y. A
cen
tury
ag
o i
t st
art
ed
an
d I
th
ink
it's
very
in
tere
stin
g t
o s
ee h
ow
th
is a
ffect
s ou
r p
erc
ep
tion
an
d o
ur
view
of
the
worl
d..
. p
hys
icall
y.
49
.
Rein
hard
So d
o y
ou
see t
his
rath
er
as
a p
rob
lem
or
som
e m
oti
vati
on
to g
o a
head
an
d d
oso
me t
hin
gs?
50
.
Flo
rian
It i
s ra
ther
a m
oti
vati
on
to u
nd
ers
tan
d.
Th
is b
att
le b
etw
een
reali
sts
an
d l
oca
ln
on
-reali
sts
is q
uit
e f
asc
inati
ng
. B
eca
use
rig
ht
now
it
is b
eco
min
g h
ard
to fi
nd
ag
uy
wh
o b
eli
eve
s in
loca
l h
idd
en
vari
ab
le t
heori
es
[th
e E
PR
pap
er
arg
ues
for
those
], o
r eve
n n
on
-loca
l h
idd
en
vari
ab
le t
heori
es
[Boh
m's
th
eory
is
on
e o
f th
ose
].To m
e p
ers
on
all
y th
is l
ooks
like p
eop
le t
ryin
g t
o k
eep
th
e o
ld w
ay
of
lookin
g a
tth
ing
s. N
ot
makin
g t
he s
tep
nece
ssary
to u
nd
ers
tan
d q
uan
tum
mech
an
ics.
51
.
Rein
hard
Th
e q
uest
ion
is
how
far
it r
eall
y m
att
ers
? A
s yo
u s
aid
befo
re a
t th
e e
xperi
men
t,ri
gh
t n
ow
, it
is
qu
ite c
lass
ical.
52
.
Flo
rian
For
me t
hat
was
the m
oti
vati
on
to c
om
e h
ere
. I
kn
ow
th
at
I'm
not
rese
arc
hin
g i
nth
is d
irect
ion
. S
o I
'm d
oin
g c
lass
ical
ph
ysic
s [s
arc
asm
]. T
he h
op
e o
f th
eexp
eri
men
t is
to g
o r
eall
y in
th
e q
uan
tum
reg
ime.
Bu
t it
is
a l
on
g w
ay.
An
d i
t's
act
uall
y a c
hall
en
ge.
I d
on
't t
hin
k a
nyb
od
y w
ou
ld d
ou
bt
that
it w
ill
not
work
, b
ut
it's
an
are
a o
f p
hys
ics
that
has
not
been
test
ed
.
53
.
Rein
hard
At
least
you
have
to d
o t
he t
hin
gs.
Pro
posi
ng
is
qu
ite o
k,
bu
t at
som
eti
me y
ou
'dli
ke t
o,
at
least
, sh
ow
or
see t
hat
there
is
som
eth
ing
.5
4.
An
d d
o y
ou
th
ink t
hat
exp
eri
men
ts h
elp
? If
you
th
ink o
f it
pers
on
all
y th
at
you
get
ab
ett
er
idea a
bou
t th
e s
itu
ati
on
?5
5.
Flo
rian
You
mean
rela
tive
to q
uan
tum
mech
an
ics?
56
.R
ein
hard
Yeah
. Yo
u g
et
more
acc
ust
om
ed
to i
t?5
7.
Flo
rian
So w
ith
th
is c
urr
en
t exp
eri
men
t, n
o.
Defi
nit
ely
not.
Fro
m t
he t
heory
I r
ead
, th
eth
eory
pap
ers
I r
ead
, I
get
a b
it.
I g
uess
I s
till
in
crease
my
un
ders
tan
din
g o
f th
eth
ing
s th
rou
gh
in
tera
ctio
ns
wit
h o
ther
peop
le f
rom
th
e q
uan
tum
gro
up
.
58
.
Rein
hard
So i
t is
more
lik
e t
he e
xch
an
ge o
f th
e v
iew
s th
at
are
cir
cula
tin
g a
rou
nd
here
th
at.
..5
9.
Flo
rian
An
d I
th
ink e
ven
th
ou
gh
we a
re n
ot.
.. I
th
ink t
he c
om
mon
dete
rmin
itor
of
eve
ryb
od
y in
th
e q
uan
tum
gro
up
is
an
in
tere
st f
or
this
kin
d o
f th
ing
s. E
ven
if
the
syst
em
s w
e a
re d
eali
ng
wit
h a
re n
ot
the s
am
e,
we c
an
alw
ays
fin
d a
gro
un
d f
or
dis
cuss
ion
s.
60
.
C Transcription of Interviews
128
Rein
hard
Do y
ou
have
an
y id
ea o
r...
Wh
at
wou
ld y
ou
th
ink w
ou
ld m
ake i
t easi
er
tou
nd
ers
tan
d q
uan
tum
mech
an
ics?
Do y
ou
see a
kin
d o
f h
op
e t
hat
there
wil
l b
e s
om
ech
an
ges
so t
hat
you
get
som
e e
asy
acc
ess
?
61
.
Flo
rian
Th
e o
nly
way
I th
ink i
t ca
n..
. U
nle
ss t
here
is
a b
ig c
han
ge t
o q
uan
tum
mech
an
ics
an
d t
here
is
a b
ig c
han
ge i
n t
he t
heory
, b
eca
use
we f
ou
nd
som
e w
ay
to e
xpla
in i
t.O
r to
get
the s
am
e r
esu
lts
wit
hou
t re
sort
ing
to t
he w
ave
fu
nct
ion
. I
thin
k t
he
chan
ge t
hat
mig
ht
hap
pen
is
on
ly a
t th
e p
ed
ag
og
ical
leve
l. P
eop
le l
earn
ing
it
diff
ere
ntl
y. H
avi
ng
acc
ess
to m
ore
exa
mp
les.
I t
hin
k t
he e
xperi
men
ts t
hat
have
hap
pen
ed
in
In
nsb
ruck
an
d V
ien
na i
n t
he l
ast
tw
en
ty y
ears
are
good
exa
mp
les
that
can
be u
sed
to l
earn
more
ab
ou
t q
uan
tum
...
To g
et
a b
igg
er
gra
sp o
f q
uan
tum
mech
an
ics.
62
.
Rein
hard
So i
t is
more
lik
e a
tech
nolo
gic
al
pro
gre
ss?
63
.F
lori
an
I w
as
not
speakin
g o
f th
e t
ech
nolo
gic
al
pro
gre
ss.
I w
as
just
th
inkin
g o
f b
asi
call
yth
e r
eali
sati
on
of
Ged
an
ken
exp
eri
men
ts.
Th
at
this
reall
y w
ork
s. A
nd
you
have
man
y d
iffere
nt
ways
of
makin
g t
he e
xperi
men
t w
ork
. Yo
u h
ave
man
y d
iffere
nt
syst
em
s. A
nd
th
ey
all
ag
ree w
ith
qu
an
tum
mech
an
ics.
Fro
m a
ll o
f th
ose
diff
ere
nt
syst
em
s, y
ou
can
som
eh
ow
make a
bett
er
pic
ture
in
you
r h
ead
.
64
.
Rein
hard
As
you
alr
ead
y sa
id.
Fro
m y
ou
r ty
pe o
f ed
uca
tion
you
had
, d
id y
ou
fin
d s
om
eth
ing
lack
ing
? B
eca
use
you
said
th
at
more
pri
vate
ly y
ou
got
inte
rest
ed
in
th
ese
kin
d o
fth
ing
s, o
uts
ide o
f st
ud
yin
g p
hys
ics.
65
.
Flo
rian
I h
ave
to s
ay
it i
s m
ore
a p
ers
on
al
thin
g.
Bu
t I
thin
k i
t w
as
lack
ing
, b
eca
use
I'm
inte
rest
ed
in
it.
We a
lso d
idn
't h
ave
an
y co
urs
es
on
pla
sma p
hys
ics.
I'm
less
inte
rest
ed
in
th
at,
so..
. I
had
th
e b
asi
s to
go o
n a
nd
seek q
uan
tum
in
form
ati
on
.W
hat
was
mis
sin
g f
rom
th
e c
ou
rses
was
just
th
e d
efi
nit
ion
of
qu
an
tum
en
tan
gle
men
t ri
gh
t aw
ay.
We k
new
[??
? a w
ord
I c
ou
ld n
ot
get
???]
, w
e k
new
den
sity
matr
ices,
we k
new
eve
ryth
ing
th
at
lead
s u
p t
o t
hat
poin
t. W
e n
eve
r h
ad
ab
ipart
ite s
yste
m [
syst
em
of
two p
art
s; c
an
sp
ort
en
tan
gle
men
t or
not]
desc
rib
ed
an
d t
hen
sh
ow
you
th
at
you
can
have
sta
tes
that
are
not
sep
ara
ble
[i.
e.
that
the a
reen
tan
gle
d].
66
.
Rein
hard
Th
is i
s a v
ery
basi
c le
vel
of
qu
an
tum
mech
an
ics.
67
.F
lori
an
Yeah
, of
qu
an
tum
in
form
ati
on
.6
8.
Rein
hard
Oh
yeah
, q
uan
tum
in
form
ati
on
.6
9.
Flo
rian
So i
n q
uan
tum
mech
an
ics
we w
en
t m
ore
in
th
e d
irect
ion
of
qu
an
tum
field
th
eory
[th
eory
ab
ou
t q
uan
tum
sys
tem
s cl
ass
icall
y re
pre
sen
ted
by
an
in
fin
ite n
um
ber
of
dyn
am
ical
deg
rees
of
freed
om
(fi
eld
s)],
or
part
icle
ph
ysic
s. T
hat
is w
hy
I le
arn
ed
alo
t ab
ou
t p
ath
in
teg
rals
an
d t
hin
gs
like t
hat.
Wh
ich
is
als
o a
dva
nce
d s
tuff
. I
thin
kth
e q
uan
tum
in
form
ati
on
stu
ff i
s m
ore
easy
to g
rasp
, b
eca
use
it
has
less
math
em
ati
cs b
eh
ind
it.
On
ce y
ou
have
th
e b
asi
s of
qu
an
tum
mech
an
ics.
.. S
o y
ou
can
act
uall
y u
nd
ers
tan
d q
uit
e e
asi
ly o
pen
pro
ble
ms.
You
can
easi
ly g
o t
o o
pen
pro
ble
ms
from
a b
asi
c...
Th
at
does
not
mean
you
can
solv
e t
hem
.
70
.
Rein
hard
Bu
t yo
u a
re g
ett
ing
th
ere
qu
ite q
uic
k i
n r
esp
ect
to o
ther
field
s of
scie
nce
, w
here
71
.
you
have
to g
o t
hro
ug
h a
lot
of
theore
tica
l co
nce
pts
. Ju
st t
o g
et
near
som
eth
ing
wh
ere
you
can
make s
om
eth
ing
new
or
have
id
eas
ab
ou
t h
ow
exp
eri
men
ts c
ou
ldlo
ok l
ike.
Flo
rian
I th
ink t
hat'
s als
o q
uit
e a
ttra
ctiv
e i
n t
his
field
. W
hen
you
look a
t th
e f
ou
nd
ati
on
s,th
en
you
wil
l n
eve
r lo
ok a
t a v
ery
com
pli
cate
d s
yste
m.
We a
lways
try
to m
ake i
t as
sim
ple
as
poss
ible
. A
nd
as
cou
nte
r-in
tuit
ive a
s p
oss
ible
, in
th
e c
ase
of
the
fou
nd
ati
on
s of
qu
an
tum
mech
an
ics.
72
.
tech
nis
ch
er
Fort
sch
ritt
Rein
hard
How
do y
ou
see t
he t
ech
nic
al
pro
gre
ss;
how
far
you
r in
sig
ht
goes?
73
.F
lori
an
For
exp
eri
men
ts t
he t
ech
nic
al
pro
gre
sses
are
sim
ple
wh
at
all
ow
s u
s to
make b
ett
er
exp
eri
men
ts.
In a
sen
se i
t is
reall
y im
port
an
t. W
e d
on
't d
o a
lot
of
ap
pli
ed
rese
arc
h,
bu
t w
e d
efi
nit
ely
need
oth
er
peop
le t
o d
o i
t. T
o g
et
bett
er
dete
ctors
,b
ett
er
ele
ctro
nic
s, b
ett
er
op
tica
l co
mp
on
en
ts.
We a
re o
nly
try
ing
to u
se a
ll t
he
new
est
an
d b
est
toys
th
at
we c
an
bu
y.
74
.
Inte
rpre
tati
on
/ T
heori
e /
Exp
eri
men
t
Rein
hard
In r
esp
ect
to i
nte
rpre
tati
on
s of
qu
an
tum
mech
an
ics,
do t
hey
mean
an
yth
ing
to
you
? T
hey
mig
ht
not
matt
er
in t
he e
xperi
men
t. O
f co
urs
e n
ot.
Wh
en
you
are
in
th
ela
b a
nd
doin
g t
hin
gs.
.. B
ut
at
wh
at
stag
e,
if a
t all
, d
o y
ou
min
d a
bou
t th
em
?
75
.
Flo
rian
So I
don
't m
ind
ab
ou
t th
em
. I
thin
k i
t is
act
uall
y g
ood
to l
ook f
or
new
on
es.
Act
uall
y I'
m a
bit
relu
ctan
t to
look a
t in
terp
reta
tion
s. A
ll o
f th
em
are
fall
ing
in
toth
is c
ate
gory
: T
hey
are
not
reall
y p
red
icti
ve.
To m
e t
hey
are
in
tere
stin
g o
nly
as
aw
ay
to t
hin
k a
bou
t th
eori
es
that
cou
ld h
ave
a d
iffere
nt
pre
dic
tion
th
an
qu
an
tum
mech
an
ics.
I t
hin
k t
hey
are
use
ful.
Ju
st a
s a t
ool
to t
hin
k a
bou
t w
hat
cou
ld c
han
ge
in q
uan
tum
mech
an
ics.
Wh
at
mod
ifica
tion
s co
uld
be m
ad
e t
o q
uan
tum
mech
an
ics
an
d t
hen
how
to t
est
th
em
. B
ut
pers
on
all
y I
don
't h
ave
str
on
g f
eeli
ng
s ab
ou
t an
y of
them
. I'
m b
asi
call
y m
ore
pra
gm
ati
st.
76
.
Rein
hard
If t
hey
are
not
pre
dic
tin
g a
nyt
hin
g,
how
cou
ld t
hey
pla
y a b
ig r
ole
?7
7.
Flo
rian
I m
ean
th
ey
cou
ld p
lay
a b
ig r
ole
in
th
e w
ay
we s
ee o
r te
ach
qu
an
tum
mech
an
ics.
Bu
t I
thin
k t
hey
are
all
a b
it m
ore
...
It i
s an
ext
ra l
aye
r of
info
rmati
on
on
top
of
the
stu
ff t
hat
you
reall
y n
eed
to k
now
to d
o q
uan
tum
mech
an
ics.
I'm
alw
ays
tem
pte
dto
learn
more
ab
ou
t th
em
, ju
st t
o fi
nd
th
e d
iffere
nce
s. I
th
ink t
hey
reall
y h
ave
an
imp
act
on
th
e w
ay
we p
op
ula
rize
sci
en
ce o
r q
uan
tum
mech
an
ics.
If
you
take t
he
man
y-w
orl
ds
theory
, th
at
is a
very
str
on
g w
ay
to i
nsi
st o
n t
he p
ecu
liari
ties
of
qu
an
tum
mech
an
ics.
Bu
t, i
t is
als
o a
nic
e w
ay
to p
inp
oin
t th
e m
easu
rem
en
tp
rob
lem
.
78
.
Rein
hard
So i
t is
a q
uest
ion
of.
.. I
f yo
u e
xag
gera
te t
he p
oin
t th
at
there
is
the m
easu
rem
en
tp
rob
lem
or
you
don
't?
79
.
Flo
rian
Th
at
is a
ctu
all
y a g
ood
poin
t. I
t is
a w
ay
to e
xag
gera
te i
t.8
0.
Rein
hard
129
Cou
ld I
th
ink o
f so
meth
ing
els
e?
Let
me s
ee.
Pro
bab
ly n
ot.
So i
f yo
u w
an
t to
ad
dso
meth
ing
? S
om
eth
ing
I d
idn
't m
en
tion
?8
1.
Flo
rian
Sorr
y th
at
I d
on
't h
ave
a l
ot
of
han
ds-
on
exp
eri
men
ts w
ith
en
tan
gle
men
t ri
gh
t n
ow
.If
you
have
qu
est
ion
s la
ter
you
can
alw
ays
sen
d a
n e
or.
..8
2.
Rein
hard
So,
than
k y
ou
very
mu
ch f
or
the i
nte
rvie
w.
83
.(n
o s
peaker)
small
talk
84
.
C Transcription of Interviews
130
Mark
us_
110706
Inte
rvie
w m
it M
ark
us
Asp
elm
eye
r vo
m 0
6.0
7.2
01
1T
ran
scri
bed
by
yott
a,
vers
ion
2 o
f 1
10
70
8
An
fan
g,
pers
ön
lich
e D
ate
n,
Au
sbil
du
ng
(no s
peaker)
[sm
all
talk
]1
.R
ein
hard
Ich
werd
e v
ers
uch
en
es
wie
bei
all
en
an
dere
n z
u m
ach
en
; all
en
an
dere
nIn
terv
iew
s. A
llg
em
ein
e F
rag
en
: W
ie a
lt b
ist
du
?2
.
Mark
us
[lach
t] D
a m
uss
ich
selb
er
imm
er
nach
den
ken
. 3
7.
Wart
e.
Ja.
Irg
en
dw
an
n h
ört
man
zu z
äh
len
au
f.3
.
Rein
hard
Ja,
ja.
Das
hab
e i
ch s
chon
öft
ers
geh
ört
.4
.M
ark
us
Dan
n s
chätz
t m
an
ein
fach
.5
.R
ein
hard
Reic
ht
ja.
6.
Wie
war
dein
e A
usb
ild
un
g?
Od
er
sag
en
wir
so,
wo h
ast
du
stu
die
rt?
Wie
ist
es
dan
n e
in b
isse
rl w
eit
erg
eg
an
gen
? S
pezi
ell
er
dan
n i
n R
ich
tun
g:
Wie
bis
t d
u z
ur
Qu
an
ten
mech
an
ik g
ekom
men
, od
er
dem
Feld
, sa
gen
wir
so?
7.
Mark
us
Als
o s
tud
iert
hab
e i
ch i
n M
ün
chen
, an
der
LM
U,
Ph
ysik
. U
nd
an
der
Hoch
sch
ule
für
Ph
iloso
ph
ie,
Ph
iloso
ph
ie.
Als
o z
uers
t n
ur
Ph
ysik
un
d d
an
n a
b d
em
sech
sten
,si
eb
ten
Sem
est
er
in d
er
Ph
ysik
hab
e i
ch d
an
n P
hil
oso
ph
ie a
ng
efa
ng
en
. H
ab
e d
an
nir
gen
dw
an
n m
ein
Dip
lom
in
der
Ph
ysik
gem
ach
t u
nd
mein
Bakkala
ure
at
in d
er
Ph
iloso
ph
ie.
Bei
Balz
er
[Wolf
gan
g B
alz
er]
mein
e W
isse
nsc
haft
theori
e i
mN
eb
en
fach
gem
ach
t. D
as
war
gan
z lu
stig
. U
nd
bin
...
Hab
e d
an
ach
dan
n m
ein
eP
rom
oti
on
in
der
Ph
ysik
an
gefa
ng
en
. D
as
war
in d
er
Fest
körp
erp
hys
ik.
Ich
hab
eein
Dip
lom
sch
on
in
der
Fest
körp
erp
hys
ik g
em
ach
t u
nd
zw
ar
war
ich
da i
nH
ou
ston
fü
r ein
ein
halb
Jah
re;
mit
Sim
on
Moss
. H
ab
e d
a m
ein
e D
iplo
marb
eit
gem
ach
t, e
xperi
men
tell
. U
nd
hab
e d
a a
m s
elb
en
Th
em
a w
eit
erg
earb
eit
et;
als
oü
ber
stru
ktu
rell
e P
hase
nü
berg
än
ge i
n K
rist
all
en
. M
art
en
siti
sch
e P
hase
nü
berg
än
ge
un
d f
err
oele
ktr
isch
e P
hase
nü
berg
än
ge.
8.
Hab
e d
an
n a
lso m
ein
e D
okto
rarb
eit
gem
ach
t in
Mü
nch
en
an
der
LM
U b
eim
Peis
l[J
oh
an
n P
eis
l] u
nd
war
als
o o
ft d
a i
n H
ou
ston
. U
nd
an
Syn
chro
tron
s[T
eil
chen
besc
hle
un
iger]
au
f d
er
gan
zen
Welt
, w
eil
das
hau
pts
äch
lich
Un
ters
uch
un
g v
on
die
sen
Kri
stall
eig
en
sch
aft
en
, vo
n d
iese
n P
hase
nü
berg
än
gen
...
Den
n e
s g
ing
um
Ph
ase
nü
berg
än
ge b
ei
den
en
sic
h d
ie G
itte
kon
stan
te [
Para
mete
r(L
än
gen
an
gab
e,
Win
kel)
zu
r B
esc
hre
ibu
ng
ein
es
Git
ters
, in
sbeso
nd
ere
der
kle
inst
en
Ein
heit
des
Git
ters
, d
er
Ele
men
tarz
ell
e]
än
dert
.
9.
Rein
hard
Ah
ok.
D.h
. d
ie z
u m
ess
en
.1
0.
Mark
us
Gen
au
, d
ie z
u v
erm
ess
en
mit
vers
chie
den
en
Meth
od
en
un
d z
u v
ers
teh
en
. U
nd
hab
e d
an
n 2
00
2 a
bg
esc
hlo
ssen
; d
ie D
iss.
Hab
e n
eb
en
bei
dan
n a
ng
efa
ng
en
...
Hab
ed
ie Z
ula
ssu
ng
mir
geh
olt
fü
r ein
e D
iss
in d
er
Ph
iloso
ph
ie.
War
offi
ziell
dan
n s
chon
ein
gesc
hri
eb
en
als
Dokto
ran
d b
ei
den
Ph
iloso
ph
en
. W
ar
gera
de s
o a
uf
11
.
Th
em
en
such
e.
Hab
e m
it B
luth
rup
p [
???]
un
d s
o w
eit
er
verh
an
delt
, w
as
man
dan
nd
a m
ach
en
kön
nte
. U
nd
hab
e a
ber
neb
en
bei
dan
n a
uch
gesc
hau
t, w
as
sin
d s
ow
eit
ere
Mög
lich
keit
en
in
der
Ph
ysik
. U
nd
da g
ab
s vi
ele
Mög
lich
keit
en
in
der
Fest
körp
erp
hys
ik w
eit
erz
um
ach
en
.U
nd
all
erd
ing
s h
ab
e i
ch m
ich
au
ch g
efr
ag
t: W
äre
es
jetz
t n
ich
t ein
e g
ute
Gele
gen
heit
ein
mal
was
an
dere
s zu
mach
en
? U
nd
die
rati
o w
ar
gan
z ein
fach
. Ic
hh
ab
e m
ich
gefr
ag
t, w
as
ist
das
was
mic
h a
m m
eis
ten
in
tere
ssie
rt u
nd
worü
ber
ich
am
wen
igst
en
weiß
. U
nd
die
Üb
erl
eg
un
g w
ar
ein
fach
. W
en
n m
an
sic
h n
ich
tau
sken
nt
mit
etw
as,
dan
n m
uss
man
ein
fach
an
fan
gen
au
f d
em
Geb
iet
zu a
rbeit
en
.Ja
, als
o d
ie Q
uan
ten
ph
ysik
war
seit
jeh
er
mein
Ste
cken
pfe
rd,
au
ch w
äh
ren
d d
es
Stu
diu
ms.
Ich
gla
ub
e d
as
geh
t ein
em
jed
en
so d
er
irg
en
dw
ie a
n G
run
dla
gen
inte
ress
iert
ist
, d
ass
er
an
die
sen
Fra
gen
stell
un
gen
hän
gen
ble
ibt.
12
.
Un
d d
am
it w
ar
die
ers
te F
rag
e b
ean
twort
et.
Un
d d
ie z
weit
e F
rag
e w
ar
dan
nn
atü
rlic
h,
wie
ste
llt
man
es
an
. Ic
h h
att
e d
an
n d
as
Glü
ck,
dass
der
Zeil
ing
er
[An
ton
Zeil
ing
er]
dan
n m
ich
gen
om
men
hat
als
Post
-Doc,
ob
woh
l ic
h ü
berh
au
pt
kein
eVorb
ild
un
g i
n d
er
Qu
an
ten
op
tik,
wh
ats
oeve
r, h
att
e. D
as
war
rein
es
Glü
ck.
Un
dd
an
n,
ja d
am
it g
ing
's l
os
mit
der
Qu
an
ten
ph
ysik
. S
eit
dem
bin
ich
in
Wie
n u
nd
so
weit
er.
13
.
Rein
hard
Seit
dem
läu
ft d
as.
Un
d s
eit
wan
n h
ast
du
sozu
sag
en
die
Gru
pp
e?
14
.M
ark
us
Als
o w
ir h
ab
en
...
Ich
hab
e d
an
n s
eh
r vi
el
gele
rnt
vom
An
ton
[A
nto
n Z
eil
ing
er]
un
din
An
ton
's G
rup
pe s
eh
r vi
el
Ph
oto
nen
exp
eri
men
te g
em
ach
t. U
nd
bin
dan
n m
it i
hm
an
das
Akad
em
ie I
nst
itu
t, d
as
Inst
itu
t fü
r Q
uan
ten
op
tik u
nd
Qu
an
ten
info
rmati
on
[ÖA
W,
IQO
QI]
, g
eg
an
gen
. 2
00
4 w
ar
das,
20
05
. U
nd
das
war
dan
n a
uch
die
Zeit
als
wir
an
gefa
ng
en
hab
en
ers
tmals
üb
er
die
se m
ech
an
isch
en
Sys
tem
e n
ach
zud
en
ken
. U
nd
ob
man
da n
ich
t m
it d
er
Qu
an
ten
op
tik s
ow
as
wie
Vers
chrä
nku
ng
un
d s
o w
eit
er
err
eic
hen
kan
n.
15
.
Un
d d
a h
ab
e i
ch d
an
n a
ng
efa
ng
en
die
Exp
eri
men
te h
och
zuzi
eh
en
. A
lso d
er
An
ton
[An
ton
Zeil
ing
er]
hat
die
urs
prü
ng
lich
mit
fin
an
ziert
un
d h
at
natü
rlic
h a
uch
mit
dis
ku
tiert
am
An
fan
g.
Hat
mir
ab
er
im P
rin
zip
völl
ig f
reie
Han
d g
ela
ssen
, als
oin
der
Au
swah
l d
er
Leu
te u
nd
in
der
Art
un
d W
eis
e w
ie w
ir d
as
Exp
eri
men
th
och
zieh
en
. Ja
, u
nd
so i
st e
s d
an
n p
ass
iert
. W
ir h
ab
en
dan
n 2
00
6 d
ie e
rste
nA
rbeit
en
pu
bli
ziert
. F
ür'
s ers
te L
ase
rkü
hlu
ng
zu
r M
ech
an
ik g
em
ach
t. D
as
gin
gw
eit
er
un
d i
m P
rin
zip
...
Da k
am
en
au
ch d
ie e
rste
n D
ritt
mit
tel
un
d i
ch h
ab
e d
an
nd
am
it i
m P
rin
zip
die
gan
ze F
ors
chu
ng
selb
st fi
nan
ziert
, au
s eig
en
en
Mit
teln
. D
as
war
so a
b 2
00
6.
Un
d d
an
n 2
00
9 g
ab
es
dan
n e
in p
aar
Ru
fe a
n U
niv
ers
itäte
n,
un
ter
an
dere
m W
ien
. O
xford
un
d C
alg
ary
hab
e i
ch d
an
n a
bg
ele
hn
t. W
ien
hab
e i
chan
gen
om
men
. S
eit
dem
bin
ich
au
f d
er
Un
i.
16
.
Rein
hard
Üb
er
die
Brü
cke g
eg
an
gen
un
d..
. [I
QO
QI
un
d d
as
Ph
ysik
inst
itu
t si
nd
in
zw
ei
Geb
äu
den
gle
ich
neb
en
ein
an
der,
verb
un
den
du
rch
ein
e F
uß
gän
gerb
rück
e].
17
.
Mark
us
Seit
Ap
ril
20
11
offi
ziell
hab
en
wir
säm
tlic
he L
ab
ors
um
gezo
gen
un
d s
ind
voll
stän
dig
au
f d
er
Un
ivers
ität.
[lach
t]1
8.
Rein
hard
Voll
stän
dig
das
Geb
äu
de g
ew
ech
selt
.1
9.
Mark
us
Ein
ein
halb
Jah
re g
ed
au
ert
, ab
er
imm
erh
in.
Ok,
sovi
el
zur
ku
rzen
vit
a.
20
.
Au
fgab
e i
m E
xp
eri
men
t /
Roll
e i
n d
er
Gru
pp
e
Rein
hard
131
Gen
au
. K
urz
e F
rag
e,
weil
ich
das
au
ch d
ie a
nd
ere
n g
efr
ag
t h
ab
e.
Was
ist
dein
Job
,so
zusa
gen
? D
ein
han
ds-
on
...?
[la
cht]
21
.
Mark
us
Ja,
gu
te F
rag
e.
Ich
vers
uch
e m
ein
e Z
eit
an
der
Un
i zu
nu
tzen
um
mög
lich
st v
iel
mit
den
Leu
ten
in
mein
er
Gru
pp
e z
u i
nte
rag
iere
n.
Ich
vers
uch
e i
ns
Lab
or
zu g
eh
en
un
d d
ort
zu
helf
en
wo g
eh
t. I
ch v
ers
uch
e d
ie F
inan
zieru
ng
all
er
Exp
eri
men
te a
mL
eb
en
zu
erh
alt
en
. Ic
h v
ers
uch
e n
eu
e I
mp
uls
e z
u g
eb
en
. E
infa
ch n
eu
e R
ich
tun
gen
zu d
efi
nie
ren
. Ja
, u
nd
dam
it i
st d
er
Tag
dan
n s
chon
au
sgefü
llt.
Ich
vers
uch
eh
au
pts
äch
lich
blö
d d
ah
er
zu r
ed
en
.[la
cht]
22
.
Rein
hard
Als
o f
un
kti
on
iert
das
noch
, d
ass
du
in
s L
ab
or
kom
mst
un
d..
.?2
3.
Mark
us
Ja,
was
sich
zeit
lich
nim
mer
au
sgeh
t, l
eid
er
Gott
es,
ist
, d
ass
man
so v
ier,
fü
nf
Stu
nd
en
am
Stü
ck,
ein
fach
mal
zur
Just
ag
e v
erw
en
det.
Das
fun
kti
on
iert
desw
eg
en
nic
ht,
weil
es
nic
ht
dam
it g
eta
n i
st,
dass
man
ein
mal
vier,
fü
nf
Stu
nd
en
am
Stü
cksi
ch h
inst
ell
t, s
on
dern
das
mu
ss m
an
kon
stan
t m
ach
en
. U
nd
das
ist
die
se K
on
stan
zd
ie f
eh
lt.
Als
o,
ich
kan
n m
ir d
urc
hau
s d
iese
Zeit
neh
men
. U
nd
das
mach
en
, ein
mal.
Ja,
ab
er
dan
n i
st a
m n
äch
sten
Tag
sch
on
wie
der
was
an
ders
. B
zw.
die
näch
sten
vier,
fü
nf
Stu
nd
en
, w
o m
an
dan
n K
on
tin
uit
ät
hab
en
mü
sste
. A
lso d
iese
Art
von
Kon
tin
uit
ät
im L
ab
or
ist
ein
bis
serl
verl
ore
n g
eg
an
gen
. A
ber
die
erk
äm
pft
man
sic
hso
Sch
ritt
fü
r S
chri
tt w
ied
er.
.. o
der
vers
uch
t si
e s
ich
wie
der
zurü
ck z
u k
äm
pfe
n.
24
.
Als
o d
e f
act
o b
in i
ch i
m P
rin
zip
im
Lab
or
um
dort
halt
mit
den
Leu
ten
zu
dis
ku
tiere
n u
nd
zu
seh
en
wo i
ch h
elf
en
kan
n.
Ab
er
ich
kan
n n
ich
t d
ad
urc
h..
. A
lso
derz
eit
jetz
t n
imm
er
kon
kre
t d
ad
urc
h h
elf
en
, d
ass
ich
dan
n m
itju
stie
re.
Leid
er.
Ab
er
das
ist
ein
rein
es
Zeit
pro
ble
m.
25
.
Rein
hard
Ja.
Un
d w
ie s
chau
t d
as
so d
ie A
uss
ich
t au
s?2
6.
Mark
us
Wora
uf?
27
.R
ein
hard
Wie
das
läu
ft?
Morg
en
hat
man
dan
n d
as
fert
ige E
rgeb
nis
...
28
.M
ark
us
Das
ist
imm
er
so.[
lach
t] D
as
ist
mein
e A
ufg
ab
e d
iese
Erw
art
un
gh
alt
un
g s
tän
dig
zu
pro
jizi
ere
n.
29
.
Nein
, ic
h w
ürd
e jetz
t ein
fach
...
Ja d
as
ist
halt
Exp
eri
men
talp
hys
ik.
Das
dau
ert
halt
ein
fach
. D
a g
lau
bst
du
hast
näch
ste W
och
e d
as
Erg
eb
nis
un
d d
an
n d
au
ert
's z
wei
Jah
re.
Ab
er,
mein
Gott
, so
ist
es.
Desw
eg
en
ist
es
wic
hti
g,
dass
die
Zie
le d
ie m
an
sich
ste
ckt
un
d d
ie E
xperi
men
te d
ie m
an
mach
t, e
infa
ch s
pan
nen
de F
rag
en
ad
dre
ssie
rt. D
ass
man
au
ch s
elb
er
nic
ht
die
Moti
vati
on
dara
n v
erl
iert
.
30
.
Rein
hard
Un
d e
rreic
hb
ar
in e
inem
gew
isse
n A
usm
aß
...?
31
.M
ark
us
Zu
min
dest
mu
ss m
an
gla
ub
en
, d
ass
sie
err
eic
hb
ar
sin
d.
Man
chm
al
sch
ad
et
ein
eg
ew
isse
Naiv
ität
üb
erh
au
pt
nic
ht.
Wen
n i
ch d
ara
n d
en
ke w
ie w
ir d
ie E
xperi
men
tean
gefa
ng
en
hab
en
20
05
zu
r M
ech
an
ik.
Wie
naiv
wir
ware
n.
Was
wir
ged
ach
th
ab
en
wie
sch
nell
das
all
es
geh
t u
nd
was
wir
all
es
mach
en
kön
nen
. H
ätt
en
wir
dam
als
das
Gan
ze r
eali
stis
cher
ein
gesc
hätz
t, h
ätt
en
wir
es
viell
eic
ht
nie
mals
an
gefa
ng
en
. W
eil
wir
dan
n s
ovi
el
An
gst
davo
r g
eh
ab
t h
ätt
en
, w
as
da a
lles
au
f u
ns
zukom
mt,
dass
wir
es
gela
ssen
hätt
en
. U
nd
so i
st e
s je
tzt
stän
dig
moti
viert
, w
as
jetz
t als
näch
stes
kom
mt,
die
näch
ste H
ürd
e z
u ü
bers
pri
ng
en
. M
an
kom
mt
zwar
lan
gsa
mer
vora
n,
ab
er
man
hat
toll
e E
rfolg
e.
32
.
Th
eori
e -
Exp
eri
men
t
Rein
hard
Als
o,
dass
ist
dan
n s
ou
nd
so a
uch
die
Fra
ge:
Wie
wü
rdest
du
dan
n d
ie B
ezi
eh
un
gzu
m E
xperi
men
t se
hen
? T
heori
e -
Exp
eri
men
t. W
eil
im
En
deff
ekt
ja i
rgen
dw
an
nd
er
Sch
ritt
ist
, w
o m
an
sag
t: O
k,
jetz
t m
uss
man
es,
wen
n's
au
ch n
aiv
ist
, m
ach
en
,an
statt
es
nu
r p
ap
ierm
äß
ig z
u e
ntw
ickeln
. S
o s
oll
te e
s eig
en
tlic
h t
heore
tisc
hau
ssch
au
en
, ab
er.
..
33
.
Mark
us
Ich
gla
ub
e m
an
kan
n k
ein
e g
en
ere
lle R
eg
el
au
fste
llen
. E
s is
t oft
mals
so,
dass
die
Th
eori
e e
in g
ute
r Id
een
geb
er
ist.
Ja,
dort
wo E
xperi
men
te t
ats
äch
lich
Vorh
ers
ag
en
fals
ifizi
ere
n k
ön
nen
, m
ög
lich
erw
eis
e,
sin
d T
heori
en
natü
rlic
h i
mm
er
seh
r g
efr
ag
t.G
leic
hze
itig
ist
es
ab
er
au
ch s
o,
dass
ein
fach
neu
e e
xperi
men
tell
e M
ög
lich
keit
en
--
die
jetz
t vö
llig
un
ab
hän
gig
sin
d v
on
der
Th
eori
e -
-, e
infa
ch d
ir e
rmög
lich
en
neu
eD
ing
e z
u m
ess
en
, n
eu
e G
röß
en
zu
mess
en
od
er
mit
un
geah
nte
r A
ufl
ösu
ng
zu
mess
en
. W
o a
uf
ein
mal
ein
e e
xperi
men
tell
e E
ntw
icklu
ng
dic
h i
n e
inen
völl
ig n
eu
en
Para
mete
rbere
ich
bri
ng
t. D
a k
an
n e
s d
urc
hau
s se
in,
dass
als
o t
heori
efr
eie
sE
xperi
men
tiere
n..
. d
ich
au
f ein
mal
das
Exp
eri
men
t so
weit
nach
vorn
e b
rin
gt,
dass
dan
n w
ied
er
au
f ein
mal
ers
tmals
th
eore
tisc
he V
orh
ers
ag
en
die
exi
stie
ren
, d
an
nü
berp
rüfb
ar
werd
en
.
34
.
Rein
hard
Wäre
das
in d
em
Feld
sozu
sag
en
der
Fall
? O
der,
wü
rdest
du
seh
en
, d
ass
das
hie
r,je
tzt
kon
kre
t b
ei
der
Op
to-M
ech
an
ik,
zutr
eff
en
wü
rde?
35
.
Mark
us
Ja,
au
f je
den
Fall
.3
6.
Rein
hard
Als
o,
dass
du
so w
as
wie
'fr
ei' e
xperi
men
tiere
n k
an
nst
? B
zw.
halt
...
37
.M
ark
us
Na ja,
es
ist
im A
ug
en
bli
ck w
irkli
ch e
in s
tän
dig
es
Neh
men
un
d G
eb
en
. A
lso w
irh
ab
en
, als
Beis
pie
l...
Die
gan
ze M
eth
od
ik d
er
Seit
en
ban
dkü
hlu
ng
die
fü
r Io
nen
,zu
m B
eis
pie
l, v
erw
en
det
wu
rde,
die
kan
n m
an
jetz
t ein
fach
an
wen
den
. A
lso d
ah
ilft
's n
atü
rlic
h d
ie T
heori
e z
u v
ers
teh
en
, w
eil
man
dam
it d
ie E
xperi
men
teop
tim
iere
n k
an
n.
Gle
ich
zeit
ig k
an
n m
an
all
erd
ing
s d
iese
s K
üh
len
an
un
d f
ür
sich
zun
äch
st m
al
völl
ig u
nab
hän
gig
davo
n e
ntd
eck
en
. W
ir h
ab
en
das
ein
fach
, d
iese
sK
üh
len
, g
em
ach
t u
nd
sin
d i
m P
rin
zip
ers
t ein
Jah
r sp
äte
r d
rau
fgekom
men
, d
ass
das
eig
en
tlic
h v
öll
ig ä
qu
ivale
nt
ist
zu d
em
was
man
in
der
Ion
en
ph
ysik
sch
on
seit
zwan
zig
Jah
ren
ken
nt.
Es
zeig
t so
ein
bis
serl
die
Naiv
ität
mit
der
man
an
man
che
Sach
en
ran
geh
t u
nd
die
dan
n a
uch
notw
en
dig
ist
.
38
.
An
dere
rseit
s h
ab
en
wir
jetz
t d
urc
h E
ntw
icklu
ng
en
, w
as
jetz
t zu
m B
eis
pie
l d
er
Mic
hael
[Mic
hael
Van
ner]
gem
ach
t h
at
mit
die
sen
Id
een
, d
ass
man
du
rch
gep
uls
tes.
.. d
as
gep
uls
te B
etr
eib
en
der
op
tom
ech
an
isch
en
Cavi
ty,
die
seZ
ust
an
dst
om
og
rap
hie
[(z
ers
töru
ng
sfre
ies)
Au
slese
n d
es
Qu
an
ten
zust
an
des
ein
es
Sys
tem
s] m
ach
en
kan
n,
gib
t's
jetz
t g
an
z to
lle n
eu
e M
ög
lich
keit
en
Eff
ekte
zu
beob
ach
ten
, d
ie m
an
mit
Vorh
ers
ag
en
au
s d
er
Qu
an
ten
gra
vita
tion
verg
leic
hen
kan
n.
Das
war
vor
zwei
Woch
en
noch
nic
ht
ab
seh
bar.
Das
sin
d a
uch
völl
ig n
eu
eE
ntw
icklu
ng
en
. Im
Pri
nzi
p g
eh
t d
as
ers
t...
ist
un
d d
as
ers
t au
fgefa
llen
, als
dan
neb
en
die
ses
neu
e e
xperi
men
tell
e K
on
zep
t d
a w
ar.
Das
theore
tisc
he K
on
zep
t zu
mA
usl
ese
n,
dass
man
jetz
t exp
eri
men
tell
um
setz
en
woll
en
. A
lso jed
en
Tag
ein
en
neu
e Ü
berr
asc
hu
ng
.
39
.
Rein
hard
Ist
ja n
ich
t sc
hle
cht.
Ja?
40
.M
ark
us
C Transcription of Interviews
132
Als
o i
ch g
lau
be e
s g
ibt
kein
e e
inh
eit
lich
e,
kein
e u
niv
ers
ell
e A
ntw
ort
au
f d
as
Wech
sels
pie
l zw
isch
en
Th
eori
e u
nd
Exp
eri
men
t. O
ftm
als
ist
es
so, w
en
n d
u d
ieT
heori
e b
ess
er
vers
teh
st,
dass
du
Exp
eri
men
te e
infa
ch i
n e
ine n
eu
e R
ich
tun
gle
nken
kan
nst
, w
eil
du
man
ches
mit
dein
em
Sys
tem
mach
en
kan
nst
au
f d
as
du
vorh
er
gar
nic
ht
gekom
men
wärs
t.
41
.
Rein
hard
Man
hän
gt
dan
n v
iell
eic
ht
nic
ht
zu s
eh
r am
Tech
nis
chen
. A
n d
en
tech
nis
chen
Hü
rden
un
d h
än
gt
dort
fest
, so
nd
ern
kan
n s
ich
au
ch w
ied
er
löse
n u
nd
th
eore
tisc
hR
ich
tun
g m
ach
en
.
42
.
Mark
us
Gen
au
. D
ie T
heori
e h
ilft
du
rch
au
s ein
fach
... Ja
das
Exp
eri
men
t vo
n e
iner
Meta
-Eb
en
e z
u b
etr
ach
ten
.4
3.
Inte
rpre
tati
on
en
Rein
hard
Un
d w
ie w
ürd
e i
n d
iese
s Verh
ält
nis
dan
n s
ow
as
rein
kom
men
wie
, n
och
etw
as
meta
-eb
en
eri
ges
wie
In
terp
reta
tion
en
? [l
an
ge P
au
se]
Weil
es
ist
ja s
chon
irg
en
dw
as
was
man
zu
gru
nd
e l
eg
t, d
en
Th
eori
en
, in
dem
Vers
tän
dn
is u
nd
das
wir
kt
sich
in
gew
isse
r W
eis
e a
uch
au
fs e
xperi
men
tal
Vers
tän
dn
is a
us.
Od
er
nic
ht?
44
.
Mark
us
Na ja,
mein
Zu
gan
g z
u I
nte
rpre
tati
on
en
ist
, d
ass
das
ideale
Exp
eri
men
t ein
solc
hes
ist.
.. s
ag
en
wir
ein
sch
ön
es
Exp
eri
men
t, e
in s
olc
hes
ist,
dass
es
dir
gera
de e
rlau
bt
dein
e z
ug
run
deli
eg
en
den
An
nah
men
, d
ie a
lso h
inte
r je
der
Inte
rpre
tati
on
ste
hen
,au
f d
en
Prü
fsta
nd
zu
ste
llen
. D
esw
eg
en
gla
ub
e i
ch s
ind
die
sch
ön
sten
Exp
eri
men
teü
berh
au
pt,
sin
d b
eis
pie
lsw
eis
e B
ell
-Exp
eri
men
te.
Ja,
weil
du
in
die
sen
Exp
eri
men
ten
tats
äch
lich
Au
ssag
en
üb
er
gan
z b
asa
le A
nn
ah
men
üb
er
ph
ysik
ali
sch
e T
heori
en
erh
ält
st.
Du
test
et
nic
ht
ein
fach
die
Vorh
ers
ag
e,.
.. b
zw.
das
stim
mt
nic
ht
gan
z. D
u t
est
et
natü
rlic
h d
ie V
orh
ers
ag
e d
er
Qu
an
ten
theori
e,
die
sag
t, d
ass
die
Korr
ela
tion
sfu
nkti
on
, w
en
n d
u d
a d
iese
n W
inkel
in e
inem
vers
chrä
nkte
n Z
ust
an
d m
isst
, ein
fach
zw
ei
Wu
rzel
zwei
ist.
Als
o i
m P
rin
zip
kan
nm
an
sag
en
, n
a ja d
u t
est
est
ein
fach
die
Qu
an
ten
theori
e.
45
.
Ab
er
der
Pu
ntk
ist
, d
ass
gera
de d
iese
r Test
, d
iese
Best
äti
gu
ng
in
dem
Fall
der
Vorh
esa
ge d
er
Qu
an
ten
theori
e,
ein
e g
an
z kla
re F
als
ifizi
eru
ng
von
basa
len
Au
ssag
en
üb
er
die
zu
gru
nd
eli
eg
en
de N
atu
r d
er
Vorg
än
ge d
ir l
iefe
rt.
Ja u
nd
das
ist
ab
solu
t, d
as
ist
ab
solu
t fa
szin
iere
nd
. Ic
h p
ers
ön
lich
fin
de jed
er
soll
te s
olc
he
Exp
eri
men
te m
ach
en
. E
xperi
men
te m
üss
en
so g
est
rick
t se
in,
dass
sie
dir
erl
au
ben
gru
nd
sätz
lich
e..
. g
run
dsä
tzli
ch d
ein
Vers
tän
dn
is ü
ber
die
basa
len
An
nah
men
üb
er
die
Natu
r zu
lie
fern
. S
o s
oll
te jed
es.
.. jed
es
Gru
nd
lag
en
exp
eri
men
t so
llte
so
au
fgeb
au
t se
in.
46
.
Rein
hard
Als
o,
dass
du
dan
n w
ied
er
un
ab
hän
gig
wir
st v
on
dem
[m
ein
te h
ier
Inte
rpre
tati
on
]u
nd
vie
lleic
ht
dan
n s
päte
r, w
en
n d
u E
rgeb
nis
se v
om
Exp
eri
men
t h
ast
, n
och
ein
mal
dir
an
sch
au
en
kan
nst
: D
ie A
nn
ah
men
die
du
getr
off
en
hast
, b
zw.
die
dan
n m
itan
dere
n Ü
berl
eg
un
gen
in
Ein
kla
ng
vers
uch
st z
u b
rin
gen
.
47
.
Mark
us
Gen
au
.4
8.
Rein
hard
Von
mir
au
s d
an
n d
ie I
nte
rpre
tati
on
au
szu
tau
sch
en
un
d s
chau
en
ob
das
noch
imm
er
irg
en
dw
ie l
eb
t.4
9.
Zie
l: k
on
sist
en
te W
elt
an
sch
au
ng
Mark
us
Weil
was
ist
das
ult
imati
ve Z
iel?
--
ist
natü
rlic
h e
ine k
on
sist
en
te W
elt
an
sch
au
un
gzu
en
twic
keln
. W
om
it k
on
sist
en
t? N
a m
it d
em
Satz
der
Beob
ach
tun
gen
die
du
mach
st.
Un
d d
am
it m
uss
t d
u d
ein
e B
eob
ach
tun
gen
geg
en
üb
er
irg
en
detw
as
ab
gle
ich
en
. D
as
heiß
t im
Pri
nzi
p w
as
du
da m
ach
st..
. Ic
h g
lau
be d
as
Bell
'sch
eT
heore
m i
st d
a e
in g
ute
s B
eis
pie
l. D
u s
chau
st e
ben
was
wäre
n d
ie K
on
seq
uen
zen
,w
en
n d
ein
Welt
bil
d d
as
ein
es
lokale
n R
eali
sten
wäre
. U
nd
au
f ein
mal
merk
st d
u,
dass
dan
n d
ein
e E
rwart
un
gen
in
kon
sist
en
t si
nd
mit
dein
en
Beob
ach
tun
gen
. Ic
hg
lau
be d
as
ist.
.. A
lso w
en
n m
an
es
sch
aff
t, g
lau
be i
ch,
die
se O
ffen
heit
geg
en
üb
er
Inte
rpre
tati
on
en
zu
hab
en
, d
an
n h
at
man
es
gesc
haff
t. D
am
it i
st m
an
off
en
gen
ug
,d
ass
man
sein
e e
igen
e P
osi
tion
im
mer
wie
der
ab
klo
pfe
n k
an
n.
50
.
Rein
hard
Gib
t es
dan
n s
ow
as,
dass
man
tro
tzd
em
sch
au
en
wil
l, d
ass
es
sozu
sag
en
nu
r ein
ekon
sist
en
te,
erk
lärb
are
An
sich
t g
ibt?
Un
d n
ich
t ein
e m
ult
iple
, d
ie i
ch d
an
nzi
em
lich
gle
ich
wert
ig a
ust
au
sch
en
kan
n?
51
.
Mark
us
Un
bed
ing
t. I
ch g
lau
be d
as
ist
wah
rsch
ein
lich
ein
e g
an
z fu
nd
am
en
tale
Moti
vati
on
für
Gru
nd
lag
en
fors
chu
ng
, d
ass
man
gla
ub
t, d
ass
...
Na,
na w
ob
ei.
Neh
me i
chw
ied
er
zurü
ck.[
Pau
se]
Als
o i
ch d
en
ke s
chon
das
die
Hoff
nu
ng
ist
, d
ass
es
ein
eri
chti
ge W
elt
an
sch
au
un
g g
ibt.
Ja,
wob
ei
das
jetz
t n
ich
t im
Sin
ne e
ines
naiv
en
Reali
smu
s g
em
ein
t is
t, s
on
dern
die
Welt
an
sch
au
un
g s
elb
st k
an
n a
uch
wie
der
ein
ese
in d
ie O
ffen
heit
zu
läss
t. D
ie z
um
Beis
pie
l zu
läss
t, d
ass
es
vers
chie
den
eW
elt
an
sch
au
un
gen
gib
t. W
ob
ei
jed
er
Jesu
it d
ich
jetz
t w
ied
er
kn
üp
peln
wü
rde,
weil
das
sch
on
wie
der
ein
Wid
ers
pru
ch i
n s
ich
ist
.
52
.
Ja,
das
ist
ein
e g
ute
Fra
ge.
Als
o i
ch d
en
ke,
dass
zu
min
dest
ein
e i
mp
lizi
te A
nn
ah
me
hin
ter,
zu
min
dest
in
der
em
pir
isch
en
Wis
sen
sch
aft
, d
ie i
st,
dass
es
ein
Welt
bil
dg
ibt,
dass
man
letz
tlic
h h
era
uss
chäle
n k
an
n.
Wob
ei
ich
beto
nen
möch
te,
es
mu
ssvi
ell
eic
ht
gar
nic
ht
der
Fall
sein
. A
lso v
iell
eic
ht
ist
Kom
ple
men
tari
tät
du
rch
au
setw
as,
was
sich
bis
in
die
Ep
iste
molo
gie
zie
ht.
Kom
ple
men
tari
tät
au
ch i
m P
rin
zip
das
sich
au
f W
elt
an
sch
au
un
gen
an
wen
den
läss
t. D
ass
es
vers
chie
den
eg
leic
hw
ert
ige B
esc
hre
ibu
ng
en
gib
t d
er
Welt
, d
ie s
ich
geg
en
seit
ig a
uss
chli
eß
en
,w
eil
sie
kom
ple
men
täre
Beg
riff
e v
erw
en
den
, ab
er
sich
au
f ein
un
d d
ie s
elb
e N
atu
rb
ezi
eh
en
, ein
un
d d
as
selb
e S
ein
bezi
eh
en
. D
as
mag
sein
.
53
.
Gan
z n
aiv
es
Beis
pie
l all
ein
au
s d
er
Ph
ysik
. E
s g
ibt
dre
i, v
ier
vers
chie
den
e A
rten
letz
tlic
h Q
uan
ten
ele
ktr
od
ynam
ik z
u v
ers
teh
en
. P
fad
inte
gra
le i
st e
infa
ch e
in v
öll
igan
dere
r Z
ug
an
g a
ls a
van
ciert
e u
nd
reta
rtie
rte M
om
en
te,
un
d s
o w
eit
er.
54
.
Rein
hard
Ab
er
das
wäre
dan
n e
twas
das
man
nic
ht
du
rch
die
Betr
ach
tun
g v
on
Th
eori
en
un
dIn
terp
reta
tion
en
irg
en
dw
ie d
irekt
hera
usl
ese
n k
ön
nte
? D
ie F
rag
e i
st w
elc
he R
oll
ed
as
Exp
eri
men
t sp
ielt
? W
as
ich
mic
h f
rag
e i
st,
waru
m e
s in
letz
ter
Zeit
od
er
in d
en
letz
ten
zeh
n,
zwan
zig
Jah
ren
ein
en
gew
isse
n Z
ug
gib
t h
in i
n R
ich
tun
g,
ers
ten
s d
es
Exp
eri
men
ts u
nd
dan
n a
uch
in
Ric
htu
ng
ein
er
An
wen
du
ng
, od
er
ein
es
Um
geh
en
sso
zusa
gen
mit
den
Din
gen
? W
eil
, ic
h s
ag
e m
al,
erl
äu
tert
un
d b
esp
roch
en
sin
d s
ieau
f In
terp
reta
tion
seb
en
e s
chon
seh
r la
ng
e.
55
.
Mark
us
Was?
56
.R
ein
hard
Qu
an
ten
mech
an
ik.
57
.M
ark
us
Na ja.
Besp
roch
en
, ab
er
nic
ht
vers
tan
den
.5
8.
Kan
n E
xp
eri
men
t h
elf
en
?
133
Rein
hard
Ja,
das
ist
eb
en
die
Fra
gen
ob
jetz
t d
as
Exp
eri
men
t h
ier
helf
en
kan
n?
59
.M
ark
us
Ich
den
ke d
as
Bell
Th
eore
m i
st ja..
. D
ie B
ell
Exp
eri
men
te s
ind
ja e
in e
ind
eu
tig
er
Bele
g d
afü
r, d
ass
es
kan
n.
Wen
n d
u g
an
z kon
kre
t ein
e g
roß
e K
lass
e v
on
mög
lich
en
Welt
an
sch
au
un
gen
au
ssch
ließ
t, n
äm
lich
die
Kla
sse d
er
lokal-
reali
stis
chen
An
sch
au
un
gen
.
60
.
Rein
hard
Ja.
Als
o d
a w
äre
n w
ir s
ozu
sag
en
wie
der
bei
der
Hoff
nu
ng
hie
r im
Au
ssch
luß
sic
han
zun
äh
ern
.6
1.
Mark
us
Gen
au
. W
ob
ei
natü
rlic
h m
an
kla
r sa
gen
mu
ss,
jed
es
Exp
eri
men
t, jed
er
exp
eri
men
tell
e A
ufb
au
defi
nie
rt d
ie S
pra
che i
n d
em
ich
jetz
t m
ein
e B
esc
hre
ibu
ng
der
Natu
r fa
sse.
Als
o e
s kan
n d
urc
hau
s se
in,
dass
ich
ein
fach
...
Als
o d
ass
die
seR
ed
e v
on
Kom
ple
men
tari
tät,
das
ist
ja d
urc
hau
s etw
as
das
kom
ple
men
täre
Beob
ach
tun
gsz
ug
än
ge m
ir..
. m
ir u
nte
rsch
ied
lich
e B
esc
hre
ibu
ng
en
ein
un
d d
er
selb
en
Reali
tät
liefe
rn.
Das
kan
n d
urc
hau
s se
in.
Ab
er
wen
n i
ch m
ein
eig
en
es
wäh
le, w
ie jetz
t zu
m B
eis
pie
l d
ie Q
uan
ten
theori
e,
bzw
. je
tzt
die
se A
rt v
on
Ap
para
ten
die
ich
verw
en
de i
n d
er
Qu
an
ten
op
tik z
um
Beis
pie
l, d
an
n,
gla
ub
e i
ch,
gib
t es
nu
r ein
e k
on
sist
en
te B
esc
hre
ibu
ng
am
En
de d
es
Tag
es.
62
.
Rein
hard
Ja.
Un
d d
ie s
ozu
sag
en
du
rch
das
Exp
eri
men
t...
63
.M
ark
us
Au
f je
den
Fall
. Ja
, ja
. W
ob
ei
man
dan
n n
atü
rlic
h..
. d
an
n w
ied
er
den
Zir
kel
gem
ach
th
ab
en
un
d z
urü
ck s
ind
beim
log
isch
en
Posi
tivi
smu
s. D
an
n i
st d
as
em
pir
isti
sch
eS
inn
kri
teri
um
vie
lleic
ht
du
rch
au
s etw
as
was
selb
st f
ür
die
Meta
ph
ysik
beg
inn
tB
ed
eu
tun
g z
u h
ab
en
. A
lso d
iese
r B
eg
riff
'exp
eri
men
tell
e M
eta
ph
ysik
', d
er
ja v
on
Ab
ner
Sh
imon
y g
ep
räg
t w
ord
en
ist
, is
t au
s d
er
Sic
ht
des
Wie
ner
Kre
ises
ja s
o e
ing
ew
isse
r [P
au
se]
Wid
ers
pru
ch.
Ein
e Q
uad
ratu
r d
es
Kre
ises,
sozu
sag
en
. A
ber
gle
ich
zeit
ig k
ön
nte
das
au
ch d
ie A
ufl
ösu
ng
sein
zu
dem
Gan
zen
. E
s w
äre
inte
ress
an
t m
al
so d
en
Beg
riff
exp
eri
men
tell
e M
eta
ph
ysik
der
Qu
ine's
chen
An
aly
seg
eg
en
üb
er
zu s
tell
en
.
64
.
Rein
hard
Mm
h.
Ja.
[nach
den
kli
ches
Sch
weig
en
]6
5.
Mark
us
Ich
gla
ub
e d
as
ist
die
gro
ße L
eis
tun
g.
Es
gib
t ja
Leu
te d
ie d
urc
hau
s vo
n d
er
Kop
ern
ikan
isch
en
Wen
de,
von
der
zweit
en
Kop
ern
ikan
isch
en
Wen
de s
pre
chen
,w
en
n s
ie ü
ber
das
Bell
Th
eore
m r
ed
en
. Z
um
Beis
pie
l d
er
Bern
ard
d'E
spag
nat.
Weil
hie
r ta
tsäch
lich
in
ein
em
seh
r ein
fach
en
Exp
eri
men
t ein
e g
an
ze K
lass
e v
on
Welt
an
sch
au
un
gen
eli
min
iert
wir
d.
Un
d d
er
Wit
z is
t eb
en
, d
ass
selb
st w
en
n d
ieQ
uan
ten
theori
e z
usa
mm
en
bre
chen
wir
d u
nd
das
wir
d s
ie i
rgen
dw
an
n..
. S
elb
st i
nein
er
Nach
folg
eth
eori
e d
er
Qu
an
ten
theori
e k
an
n d
iese
Welt
an
sch
au
un
g n
ich
tw
ied
er
au
ftau
chen
, w
eil
sie
ein
fach
in
kon
sist
en
t is
t m
it d
iese
r K
lass
e v
on
Beob
ach
tun
gen
. U
nab
hän
gig
welc
he T
heori
e d
em
Gan
zen
zu
gru
nd
eli
eg
t. D
as
ist
das
eig
en
tlic
h f
asz
inie
ren
de.
66
.
Rein
hard
Das
heiß
t m
an
wü
rde e
igen
tlic
h a
uf
was
Neu
es
hoff
en
um
ein
e g
röß
ere
Kon
sist
en
zzu
hab
en
? O
der.
..6
7.
Mark
us
Na ja,
sag
en
wir
, u
m d
ie jetz
tig
en
In
terp
reta
tion
ssch
wie
rig
keit
en
mit
der
Qu
an
ten
theori
e a
us
dem
Weg
zu
räu
men
. G
en
au
.6
8.
Rein
hard
Das
sch
ein
t n
ich
t m
it b
est
eh
en
den
Den
kw
eis
en
un
d M
itte
ln m
ög
lich
?6
9.
Mark
us
Sola
ng
e w
ir n
och
so v
iele
, w
ie s
oll
ich
sag
en
, p
hän
om
en
olo
gis
ch ä
qu
ivale
nte
Inte
rpre
tati
on
en
hab
en
, u
nd
dam
it m
ein
e i
ch s
olc
he d
ie k
ein
en
off
en
sich
tlic
hen
Wid
ers
pru
ch m
it B
eob
ach
tun
gen
gen
eri
ere
n.
Sola
ng
e w
ir n
och
so v
iele
ph
än
om
en
olo
gis
ch ä
qu
ivale
nte
Welt
an
sch
au
un
gen
hab
en
, g
lau
be i
ch,
den
ken
wir
ein
fach
noch
fu
nd
am
en
tal
fals
ch.
Ich
den
ke s
chon
das
es
hie
r n
ur
ein
e g
eb
en
kan
n.
Das
heiß
t je
tzt
ist
die
Fra
ge k
ön
nen
wir
üb
er
Exp
eri
men
te h
ier
neu
es
lern
en
.W
er
weiß
.
70
.
Rein
hard
Ok,
ja.
Dass
man
das
zum
ind
est
en
s au
ch a
ls M
itte
l au
ssch
öp
fen
kan
n u
m i
n d
iese
Ric
htu
ng
zu
geh
en
.7
1.
Inkom
pati
bil
itäts
theore
me
Mark
us
Au
f je
den
Fall
. N
a,
na,
au
f je
den
Fall
. Ic
h d
en
ke d
as.
.. I
ch f
ass
e d
as
imm
er
so u
nte
rd
em
Sti
chw
ort
'In
kom
pati
bil
itäts
theore
me' zu
sam
men
. F
ür
mic
h i
st d
as
Bell
'sch
eT
heore
m e
in I
nkom
pati
bil
itäts
theore
m.
Es
ist
ein
Th
eore
m d
as
letz
tlic
h m
eh
r als
zwei
Au
ssag
en
, als
o i
n d
em
Fall
sin
d e
s als
o d
rei
Au
ssag
en
. A
uss
ag
e 1
: D
ieVorh
ers
ag
en
der
Qu
an
ten
theori
e s
ind
korr
ekt.
Au
ssag
e 2
: L
okali
täts
an
nah
me.
Au
ssag
e 3
: R
eali
smu
san
nah
me.
Un
d g
eg
eb
en
das
die
ers
te A
uss
ag
e k
orr
ekt
ist,
ist
min
dest
en
s ein
e d
er
beid
en
an
dere
n f
als
ch.
Die
se I
nkom
pati
bil
ität
ein
es
Satz
es
von
Au
ssag
en
, w
ob
ei
min
dest
en
s ein
e d
er
Au
ssag
en
exp
eri
men
tell
üb
erp
rüfb
ar
ist,
das
sin
d f
ür
mic
h I
nkom
pati
bil
itäts
theore
me.
Da g
eh
ört
das
Bell
Th
eore
m d
azu
,d
as
GH
Z-T
heore
m,
was
Leg
ett
gem
ach
t h
at
zu d
iese
r K
lass
e v
on
Nic
ht-
lokal-
reali
stis
chen
Th
eori
en
. U
nd
ste
hen
wir
noch
am
An
fan
g.
72
.
Als
o i
ch b
in m
ir s
ich
er
wir
werd
en
In
kom
pati
bil
itäts
theore
me a
uch
in
an
dere
nB
ere
ich
en
au
fste
llen
kön
nen
. A
lso i
ch d
en
ke e
ine g
an
z g
roß
e H
era
usf
ord
eru
ng
fü
rd
ie n
äch
sten
Jah
re w
ird
jetz
t se
in,
wie
sie
ht
es
mit
dem
Verh
ält
nis
...
un
ser
Vest
än
dn
is v
on
Qu
an
ten
ph
ysik
un
d G
ravi
tati
on
au
s. I
ch b
in m
ir g
an
z si
cher,
dass
hie
r d
ie G
run
dan
nah
men
, d
ie d
a jew
eil
s ein
flie
ßen
au
ch i
nkom
pati
bel
zuein
an
der
sin
d.
Un
d d
ie w
ird
man
in
In
kom
pati
bil
itäts
theore
men
letz
tlic
h a
ufs
pü
ren
.
73
.
Rein
hard
Die
dan
n w
ied
er
Exp
eri
men
te b
rau
chen
.7
4.
Mark
us
Gan
z g
en
au
. G
an
z g
en
au
. Ja
, u
nd
da w
ird
man
Fu
nd
am
en
tale
s ü
ber
en
twed
er
Qu
an
ten
ph
ysik
od
er
Gra
vita
tion
, od
er
beid
es
lern
en
. D
a b
in i
ch g
an
z fe
st d
avo
nü
berz
eu
gt.
75
.
pers
ön
lich
e M
oti
vati
on
/ F
asz
inati
on
Rein
hard
Un
d k
an
n m
an
das
au
ch a
uf
das
Pers
ön
lich
e r
un
ter
bre
chen
?7
6.
Mark
us
Mein
pers
ön
lich
es
Inkom
pati
bil
itäts
theore
m?
[lach
t]7
7.
Rein
hard
Nein
. D
as
man
au
ch p
ers
ön
lich
am
Exp
eri
men
t le
rnt
od
er
an
den
Din
gen
?7
8.
Mark
us
Au
f je
den
Fall
. Ic
h m
ein
e d
as
ist
die
Au
fgab
e d
es.
.. I
ch m
ein
e d
as
ist
jetz
t...
Ich
den
ke G
run
dla
gen
fors
chu
ng
rü
hrt
an
ein
em
zu
tiefs
t m
en
sch
lich
en
un
d e
inem
gan
zb
asa
len
men
sch
lich
en
Bed
ürf
nis
. N
äm
lich
ein
e w
iders
pru
chfr
eie
Au
ffass
un
g d
er
79
.
C Transcription of Interviews
134
all
täg
lich
en
Wah
rneh
mu
ng
en
zu
gen
eri
ere
n.
Als
o m
an
möch
te e
in..
. A
lso
men
sch
lich
e N
eu
gie
r d
ien
t d
azu
, d
ass
man
Din
ge,
die
man
erf
äh
rt w
en
n m
an
beob
ach
tet,
ein
bett
et
in e
in W
elt
bil
d.
Un
d m
an
lern
t N
eu
es
um
sein
Welt
bil
d d
an
nan
zup
ass
en
. B
zw.
Neu
es
ist
norm
ale
rweis
e g
en
au
etw
as
was
dan
n w
ied
er
leic
hte
An
pass
un
gen
an
sein
eig
en
es
Welt
bil
d i
mp
lizi
ert
. Ir
gen
dw
ie w
as
Neu
es
ist
üb
err
asc
hen
d f
ür
mic
h,
als
o w
ar
es
vorh
er
nic
ht
in m
ein
em
Welt
bil
d d
rin
. D
as
heiß
t ic
h w
erd
e d
as
en
tsp
rech
en
d a
np
ass
en
.U
nd
ich
gla
ub
e e
s is
t ein
fu
nd
am
en
tale
s m
en
sch
lich
es
Bed
ürf
nis
, b
zw.
eig
en
tlic
hso
llte
es
ein
e f
un
dam
en
tale
...
es
ist
ein
e k
on
stan
te H
era
usf
ord
eru
ng
eig
en
tlic
h a
nd
en
Men
sch
en
, d
ass
er
es
sch
aff
t all
e s
ein
e E
rfah
run
gen
in
ein
wid
ers
pru
chsf
reie
sB
ild
zu
bri
ng
en
. Ic
h fi
nd
e d
as
ist
ein
e i
nte
llektu
ell
e H
era
usf
ord
eru
ng
, ein
eem
oti
on
ale
Hera
usf
ord
eru
ng
. Ic
h h
ab
e d
as
Glü
ck,
dass
Teil
davo
n m
ein
Beru
f is
t.A
ber
ich
den
ke d
as
ist
ein
e z
uti
efs
t p
ers
ön
lich
e A
ng
ele
gen
heit
dara
n z
u a
rbeit
en
.W
eil
es
gib
t n
ich
ts p
ers
ön
lich
ere
s als
ein
wid
ers
pru
chsf
reie
s, z
um
ind
est
ein
wid
ers
pru
chsa
rmes,
Bil
d ü
ber
die
Welt
zu
gen
eri
ere
n.
80
.
Rein
hard
Un
d w
äre
das
dan
n s
ozu
sag
en
au
ch d
ein
e p
ers
ön
lich
e M
oti
vati
on
sp
ezi
ell
Qu
an
ten
mech
an
ik z
u m
ach
en
? W
eil
ja h
ier
sozu
sag
en
die
'H
era
usf
ord
eru
ng
' re
lati
vg
roß
ist
; so
zusa
gen
was
sich
dem
en
tgeg
en
stell
t kon
sist
en
t zu
sein
.
81
.
Mark
us
Gu
t, d
a s
pie
lt jetz
t n
atü
rlic
h p
ers
ön
lich
e F
asz
inati
on
mit
ein
e R
oll
e.
Jed
er
hat
sein
eeig
en
en
Vorl
ieb
en
un
d i
ch w
ar
sch
on
im
mer
von
die
sen
Fra
gest
ell
un
gen
fasz
inie
rt.
Jem
an
d a
nd
ers
der
au
f ein
em
an
dere
n G
eb
iet
fors
cht,
ist
von
an
dere
nF
rag
est
ell
un
gen
fasz
inie
rt.
Als
o f
ür
mic
h m
uss
ich
sag
en
, is
t es
ein
fach
ein
, w
iesa
gt
man
so s
chön
, a p
erf
ect
matc
h.
Un
d d
esw
eg
en
pass
t es.
Ab
er
ich
gla
ub
e m
an
soll
te n
ur
wir
kli
ch s
ich
mit
die
sen
Sach
en
, m
it s
olc
hen
Din
gen
besc
häft
igen
, d
ieein
en
wir
kli
ch b
erü
hre
n.
Weil
nu
r d
an
n h
at
man
den
Path
os
um
wir
kli
ch w
as
neu
es
zu l
ern
en
.
82
.
En
de
Rein
hard
Mm
h.
83
.M
uss
ich
fast
noch
nach
sch
au
en
.[sc
hau
e a
uf
Zett
el,
ob
ich
noch
ein
e F
rag
e h
ab
e]
Nein
.8
4.
Mark
us
War'
s d
as
sch
on
?8
5.
Rein
hard
Ja.
Von
mein
er
Seit
e a
us
wäre
ich
mit
mein
en
Fra
gen
fert
ig.
86
.M
ark
us
Su
per.
87
.R
ein
hard
Dan
ke f
ür
die
Zeit
.8
8.
Mark
us
Gern
e,
gern
e.
89
.(n
o s
peaker)
[sm
all
talk
]9
0.
135
DI(FH) Reinhard StanzlDate of Birth September 18, 1977
Nationality AustriaB [email protected]
Education09/1987 – 05/1995 Secondary School (Bundesrealgymnasium), Bruck an der Leitha.
Degree: Matriculation
Studies09/1995 – 06/1999 University of Applied Sciences Technikum Wien - Electronic Engineering
[Fachhochschul-Studiengang Elektronik], Vienna.
Thesis: “Implementierung eines Koppelfeldalgorithmus mit einer VLIW-DSP-Architektur”Degree: Graduate Engineer for Electronics [Diplom-Ingenieur für Elektronik (FH)]
03/2005 – University of Vienna, Vienna.{ Philosophy (Diploma Programme)Thesis: “On the Counter-Intuitiveness of Quantum Entanglement”{ Physics (Diploma Programme)
Professional Experience05/2000 – 03/2005 Frequentis Nachrichtentechnik GmbH, Vienna.
Systems Engineer in the Business Segment ‘TETRA’ (TErrestrial Trunked RAdio)
LanguagesGerman Native LanguageEnglish ProficientFrench Basic Knowledge
D Resume
137
E Abstract
E.1 Abstract (English)
There is a rather common dictum that quantum entanglement, a key feature of quantummechanics, is counterintuitive. This assertion can be assigned not only to laypeople, but alsoto scientists engaged in quantum mechanics. How can we make sense of this?
I elaborate the issue based on four intertwined aspects: First, on a theoretical level by intro-ducing the fundamental differences between classical physics and quantum mechanics. Thisis mainly carried out along the lines of the EPR thought experiment and the correspondingperspectives of Einstein et al. and Schrödinger. Second, on an experimental level by illus-trating the counter-intuitiveness of quantum entanglement in the context of a specific fieldof research. Namely quantum opto-mechanics, and more particularly the experimental set-up of the research group Quantum Foundations and Quantum Information on the Nano- and
Microscale at the University of Vienna. Third, on a personal level by utilizing my interviewsconducted with members of this very research group. Fourth, on a philosophical level byexploiting key concepts of Gaston Bachelard’s epistemology, such as epistemological profileor scientific reason being instructed by fabricated experience.
All of these four aspects are brought into contact to accomplish two tasks: On the one hand toflesh out the specifics and characteristics of counter-intuitiveness in the context of quantumentanglement. On the other hand to consider the question whether and how experimentingwith quantum entanglement could assist in coping with its counter-intuitiveness, for exampleby familiarization. Overall, this thesis does not provide an in-depth analysis of these twomain issues, but a plausible approach to and depiction of the subject matter.
139
E Abstract
E.2 Abstract (German)
Es gibt die verbreitete Aussage, dass Quantenverschränkung, ein Schlüsselkonzept in derQuantenmechanik, kontraintuitiv sei. Diese Behauptung kann aber nicht nur Laien zuge-schrieben werden, sondern findet sich auch bei Wissenschaftlern der Quantenmechanik wie-der. Wie können wir uns das verständlich machen?
Ich bearbeite dieses Thema auf Basis von vier miteinander verwobenen Gesichtspunkten:Erstens, auf einer theoretischen Ebene lege ich die hier relevanten Unterschiede zwischender klassischen Physik und der Quantenmechanik vor. Dies geschieht hauptsächlich anhanddes EPR Gedankenexperiments und den entsprechenden Standpunkten von Einstein et al.und Schrödinger. Zweitens, auf einer experimentellen Ebene veranschauliche ich die Kon-traintuitivität der Quantenverschränkung im Zusammenhang mit einem spezifischen For-schungsfeld. Im Konkreten erfolgt dies anhand der Quanten-Optomechanik, genauer derExperimente der Forschungsgruppe Quantum Foundations and Quantum Information on the
Nano- and Microscale der Universität Wien. Drittens, auf einer persönlichen Ebene werteich meine Interviews mit den Mitgliedern ebendieser Forschungsgruppe aus. Viertens, aufeiner philosophischen Ebene mache ich mir Schlüsselkonzepte von Gaston Bachelards Epis-temologie zunutze, wie zum Beispiel das epistemologische Profil oder einer durch Erfahrungbelehrten Vernunft.
Alle diese vier Aspekte werden zusammengenommen um zwei Aufgaben zu erfüllen: Ei-nerseits die Konkretisierung der Besonderheiten und Merkmale der Kontraintuitivität imKontext der Quantenverschränkung. Andererseits die Betrachtung der Frage ob und wie dasExperimentieren mit Quantenverschränkung den Umgang mit dessen Kontraintuitivität er-leichtert, zum Beispiel durch Gewöhnung. Im Großen und Ganzen stellt die Diplomarbeitkeine tiefgreifende Analyse dieser beiden Themen zur Verfügung, sondern liefert eine plau-sible Annäherung an das Problem.
140