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1 July 30, 2007 W. Bauer 1 Introduction History Utilization Physics Grid Mass Future Introduction History of physics & computing Use of computers in the physical sciences Examples from physics Computers at the interface of biology, chemistry and physics Use of the Internet for computing “The Road Ahead” Teaching with the Computer Wolfgang Bauer Department of Physics and Astronomy Michigan State University Theoretical / Computational Nuclear Physics July 30, 2007 W. Bauer 2 Introduction History Utilization Physics Grid Mass Future Nuclei are REALLY small Introduction Atoms are really small Typical atomic size: ~10 -10 m Put 10,000,000 atoms in a row: thickness of your fingernail Best (scanning tunneling) microscopes are just good enough to resolve individual atoms Nuclei are another factor 100,000 smaller Typical nuclear size: ~10 -15 m Nucleus inside an atom is like a golf ball in a football stadium (but contains almost all of the mass!) July 30, 2007 W. Bauer 3 Introduction History Utilization Physics Grid Mass Future How do we learn about nuclei? Introduction We hit the nuclei (with other nuclei or elementary particles or gamma rays) and watch what happens. Nuclear processes require high energy (> 1 MeV) More than 100,000 times the energy of chemical processes Nuclear processes last a very short time (<10 -21 s) A billionth of a billionth of a millisecond! Once the nuclear reaction products are detected, the reaction has long been over Direct observation of nuclei and nuclear processes is impossible We need theory to understand and model the We need theory to understand and model the experimental results and thus learn about nuclei! experimental results and thus learn about nuclei! July 30, 2007 W. Bauer 4 Introduction History Utilization Physics Grid Mass Future Nuclear Models Introduction Liquid drop model Explains basic nuclear masses Fermi gas model Independent particle motion mainly governed by Pauli principle Shell model Similar to atomic shell model Nuclear physics requires quantum mechanics, thermodynamics, fluid dynamics, transport theory, theory of phase transitions, complexity and chaos theory, …, and COMPUTERS

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Page 1: Introduction Nuclei are REALLY small Theoretical / Computational ... Theory... · Introduction History Utilization Physics Grid Mass Future Nuclei are REALLY small Introduction Atoms

1

July 30, 2007 W. Bauer 1

Introduction History Utilization Physics Grid Mass Future Introduction

History of physics & computing Use of computers in the physical

sciences Examples from physics Computers at the interface of

biology, chemistry, and physics Use of the Internet for computing Teaching with the Computer “The Road Ahead”

History of physics & computingUse of computers in the physicalsciencesExamples from physicsComputers at the interface ofbiology, chemistry and physicsUse of the Internet for computing

“The Road Ahead”Teaching with the Computer

Wolfgang BauerDepartment of Physics and Astronomy

Michigan State University

Theoretical / ComputationalNuclear Physics

July 30, 2007 W. Bauer 2

Introduction History Utilization Physics Grid Mass Future

Nuclei are REALLY smallIntroduction

Atoms are really small• Typical atomic size: ~10-10 m• Put 10,000,000 atoms in a row: thickness of your fingernail• Best (scanning tunneling) microscopes are just good enough

to resolve individual atoms Nuclei are another factor

100,000 smaller• Typical nuclear size:

~10-15 m• Nucleus inside an atom is

like a golf ball in a footballstadium (but containsalmost all of the mass!)

July 30, 2007 W. Bauer 3

Introduction History Utilization Physics Grid Mass Future

How do we learn about nuclei?Introduction

We hit the nuclei (with other nuclei or elementaryparticles or gamma rays) and watch what happens.

Nuclear processes require high energy (> 1 MeV)• More than 100,000 times the energy of chemical processes

Nuclear processes last a very short time (<10-21 s)• A billionth of a billionth of a millisecond!• Once the nuclear reaction products are detected, the

reaction has long been over• Direct observation of nuclei and nuclear processes is

impossible We need theory to understand and model theWe need theory to understand and model the

experimental results and thus learn about nuclei!experimental results and thus learn about nuclei!

July 30, 2007 W. Bauer 4

Introduction History Utilization Physics Grid Mass Future

Nuclear ModelsIntroduction

Liquid drop model• Explains basic nuclear masses

Fermi gas model• Independent particle motion mainly governed by Pauli

principle Shell model

• Similar to atomic shell model Nuclear physics requires quantum mechanics,

thermodynamics, fluid dynamics, transport theory,theory of phase transitions, complexity and chaostheory, …, and COMPUTERS

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July 30, 2007 W. Bauer 5

Introduction History Utilization Physics Grid Mass Future

Complexity in Many-Body Systems

Mesoscopic Systems: Computersbecome essential

2 !

Np

! 102!10

5

logC

Introduction

July 30, 2007 W. Bauer 6

Introduction History Utilization Physics Grid Mass Future

(very abbreviated) History of Physics

1700s1700s: Newton invents calculusto describe mechanics

1800s: Faraday et al. studyelectricity&magnetism in experiments

1900s: Theoreticalphysics (Planck,Einstein) exploresthe quantum world

2000s: Computational physics emergesas third branch of physics (von Neumann)

History

time

July 30, 2007 W. Bauer 7

Introduction History Utilization Physics Grid Mass Future

History of Computers (Moore’s Law)History

Computer speed doubles every 18 months (Moore’s Law) Data storage doubles every 12 months Network speed doubles every 9 months Improvement 1988 to 2005

(length of my MSU tenure)• Computers: x 2,500• Storage: x 130,000• Networks: x 6,600,000

Physics limits not to bereached for another decadeor more Moore’s Law vs. storage improvements vs. optical

improvements. Graph from Scientific American (Jan-2001) by Cleo Vilett, source Vined, Khoslan, Kleiner,Caufield and Perkins.

July 30, 2007 W. Bauer 8

Introduction History Utilization Physics Grid Mass Future

History of Computers (Speed Record)History

Earth Simulator

BlueGene

ASCI White

ASCI Red

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July 30, 2007 W. Bauer 9

Introduction History Utilization Physics Grid Mass Future

History of ComputersHistory

1946: ENIAC 1947: Transistor (Bardeen,Brattain, Shockley)

2000: 100 milliontransistors in each PC chip

1989: WWW, Berners-Lee, CERN 2004: BlueGene

Driven by demand from andinventions by physical scientists!

July 30, 2007 W. Bauer 10

Introduction History Utilization Physics Grid Mass Future

Use of Computers:

Utilization

Email & Office SoftwareFor all of us: significant fraction of our workday

July 30, 2007 W. Bauer 11

Introduction History Utilization Physics Grid Mass Future

Use of Computers: Programming

Utilization

Languages: FORTRAN C(++) Java

July 30, 2007 W. Bauer 12

Introduction History Utilization Physics Grid Mass Future

Use of Computers: Symbolic Manipulation

Utilization

Programs: Mathematica Maple MathLab

Real MathematicsResearch:e.g. Kepler Conjecture

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July 30, 2007 W. Bauer 13

Introduction History Utilization Physics Grid Mass Future

Use of Computers: Data Collection

Utilization

Programs: Mathematica Maple MathLab

Real MathematicsResearch:e.g. Kepler Conjecture

July 30, 2007 W. Bauer 14

Introduction History Utilization Physics Grid Mass Future

Use of Computers: Visualization

Type IA supernova explosion(BIG SPLASH)

Fusion Stellarator

Acceleratordesign

Atmospheric models

Multi-scale

model ofHIV

Materials: Quantum Corral

Collection: D. Dean, ORNL

Utilization

Nuclear Physics: STAR event (G.D. Westfall)

⇒ Insight

July 30, 2007 W. Bauer 15

Introduction History Utilization Physics Grid Mass Future

Use of Computers: Enabling Science

Utilization

Three high-tech buzzwords:

relies on advances in

Progress in

And both are dependent on

July 30, 2007 W. Bauer 16

Introduction History Utilization Physics Grid Mass Future

Computational Nano-Science

Prediction of materials’ structuresand properties

Ab initio calculations of quantumforces between atoms

Density functional theory

Physics

Example 1: Carbon pea-podmemory• U.S. Patent 6,473,351

Example 2: Time dependence ofbuckyball fusion

Calculations done with EarthSimulator

David Tomanek, MSU-PA

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July 30, 2007 W. Bauer 17

Introduction History Utilization Physics Grid Mass Future

Computational Nuclear Physics

Big questions:• How are the heaviest elements

made in the universe?• What is the equation of state of

nuclear matter? Experimental Facilities

• NSCL, (future) RIA Computational

Tools• Transport

Theory• Reaction

Networks

Physics

July 30, 2007 W. Bauer 18

Introduction History Utilization Physics Grid Mass Future

Computational Astrophysics Astrophysics has to answer questions

without any chance of doingexperiments

Running computer simulations andcomparing their output to staticobservations is only path to progress

Physics

E. Brown, with Flash Center, Chicago

July 30, 2007 W. Bauer 19

Introduction History Utilization Physics Grid Mass Future

Computing with the Internet: SETI

> 1000 CPU years/day !

~60 TeraFLOP/s

Grid

July 30, 2007 W. Bauer 20

Introduction History Utilization Physics Grid Mass Future

Large Hadron Collider@ CERN (>2008)

Computing for Data ReductionATLAS

Data storage and offline analysisATLAS: ~10 ~10 PetaByte/yearPetaByte/year (~100,000 PC hard drives of 100 GB)

Data rate: 40 MHz, 40 TB/sLevel 1 - Special hardware 75 kHz, 75 GB/sLevel 2 - embedded processors 5 kHz, 5 GB/sLevel 3 - dedicated PCs 100 Hz, 100 MB/s

Grid

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July 30, 2007 W. Bauer 21

Introduction History Utilization Physics Grid Mass Future

105

104

103

102

Even

t Rat

e (H

z)

High Level-1 Trigger(1 MHz)

High No. ChannelsHigh Bandwidth(500 Gbit/s)

High Data Archive(PetaByte)

LHCB

KLOE HERA-B TeV II

CDF/D0H1

ZEUS

UA1 NA49ALICE

Event Size (bytes)104 105 106

ATLASCMS

106

107

Parts from:Hans HoffmanDOE/NSF Review, Nov 00

Data Streams for Different Experiments

STAR

Data Rates forHigh EnergyPhysicsExperiments PHENIX

FutureCurrentMSU

Grid

July 30, 2007 W. Bauer 22

Introduction History Utilization Physics Grid Mass Future

Computing with the Internet: Grid

Grid

Tier0/1 facilityTier2 facility

10 Gbps link2.5 Gbps link622 Mbps linkOther link

Tier3 facility

InternationalVirtual GridLaboratory Graphic: Shawn McKee

2007: New MSU/UM Tier2 facility

July 30, 2007 W. Bauer 23

Introduction History Utilization Physics Grid Mass Future

One example: Nuclear MassMass

Al, here is how I see it:E=mc2

Energy and mass are related Nuclei weigh less

than the sum ofthe masses of theprotons andneutrons in them.

Nuclear binding!

July 30, 2007 W. Bauer 24

Introduction History Utilization Physics Grid Mass Future

One example: Nuclear MassMass

experimentallymeasured bindingenergies

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July 30, 2007 W. Bauer 25

Introduction History Utilization Physics Grid Mass Future

One example: Nuclear MassMass

Can we understand this? Strong force is short-ranged; nucleons only interact

with nearest neighbors No neighbors at the surface Add Coulomb repulsion between protons (+ …)

B(N ,Z ) = Bs(N ,Z ) + B

c(N ,Z ) + B

a(N ,Z ) + B

p(N ,Z )

= avA! a

sA

2/3! a

c

Z2

A1/3

! aa

Z !1

2A( )

2

A! a

p

!1( )Z

+ (!1)N

A

B(N ,Z ) / A = av! a

sA

!1/3 ! ac

Z2

A4/3

! aa

Z

A! 1

2

"#$

%&'

2

! ap

!1( )Z

+ (!1)N

A3/ 2

July 30, 2007 W. Bauer 26

Introduction History Utilization Physics Grid Mass Future

One example: Nuclear MassMass

Yep, it works!

July 30, 2007 W. Bauer 27

Introduction History Utilization Physics Grid Mass Future

One example: Nuclear MassMass

Modern picture: on closer examination differences tomass formula are revealed

Phys. Rev. C 69, 037304 (2004): Hirsch et al.

July 30, 2007 W. Bauer 28

Introduction History Utilization Physics Grid Mass Future

One example: Nuclear MassMass

Huge national effort tofind better energy densityfunctional

Leader: George Bertsch,UW

MSU has big part in thismulti-million $ effort

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July 30, 2007 W. Bauer 29

Introduction History Utilization Physics Grid Mass Future

Predictions Predictions are hard …

• “Prediction is very difficult, especially about the future”(Niels Bohr)

But still useful …• Predictions are like Austrian train schedules. Austrian trains are always

late. So why do the Austrians bother to print train schedules? How elsewould they know by how much their trains are late?(Viktor Weisskopf, paraphrased)

So here we go …• Moore’s Law will continue for at least another 2 decades• Network bandwidth will become infinitesimally cheap and eventually

(~2 decades) saturate the human input bandwidth• Caution 1: “Software is a gas” (Nathan Myhrvold)• Caution 2: Growth in content will only be linear, not exponential

Future

July 30, 2007 W. Bauer 30

Introduction History Utilization Physics Grid Mass Future

Future of Computing: Quantum Computer

Conventional computer:• N processors can process N

instructions simultaneously Quantum computer:

• N processors can process 2N

instructions simultaneously Example:

• N = 16: 216 = 65,536• N = 32: 232 = 4,294,967,296

Future collaboration potentialbetween PA, Math, CSE

Future

Proposed 16-bit quantumcomputer design: electronson liquid helium(M. Dykman et al.)

July 30, 2007 W. Bauer 31

Introduction History Utilization Physics Grid Mass Future

Summary

Physical science has provided technologicalinnovation to advance computer science and willcontinue to do so

Computers have enabled a third branch of physicalscience (besides theory and experiment)

Nuclear theory is now very dependent on large-scalecomputer use

Nuclear theory provides the only link betweenexperiments and understanding in nuclear physics