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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005 Prof. Dr. Michael Feindt CETA Institut für Experimentelle Kernphysik Universität Karlsruhe Universität Freiburg, 23. November 2005 Physics with Neural Networks Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005 Contents Hypothesis testing / classification Neural networks Classification, conditional probability densities NeuroBayes (robust regularised Bayesian neural network) Applications in DELPHI, CDF II, outside physics Unusual but powerful network applications: Training with MC/data mixtures Training on data only Training with weights Training with background subtraction Multidimensional regression using NeuroBayes

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Page 1: Physics with Neural Networksfeindt/Freiburg.pdf · Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005 Address all these topics and build a professional robust

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Prof. Dr. Michael FeindtCETAInstitut für Experimentelle KernphysikUniversität Karlsruhe

Universität Freiburg, 23. November 2005

Physics with Neural Networks

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

ContentsHypothesis testing / classificationNeural networks

Classification, conditional probability densitiesNeuroBayes (robust regularised Bayesian neural network)Applications in DELPHI, CDF II, outside physics

Unusual but powerful network applications: Training with MC/data mixturesTraining on data onlyTraining with weightsTraining with background subtraction Multidimensional regression using NeuroBayes

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Hypothesis testing

Cut in a test-statistic:Accept hypothesis H0, if t<t(cut)

Error of 1. kind:P1(true hypothesis will be rejected)

Error of 2. kind:P2(wrong hypothesis is accepted)

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Hypothesis testing

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Hypothesis testing

A statistical method is thebetter the nearer it reachesthe point (1,1) in thepurity-efficiency-plot

Optimal choice of workingpoint according to particulartask: How does the total errorof the analysis scale withε und P?

0.7 0.8 0.9 1.0

Optimalworking point

Different cuts in t

Different cuts in t

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Determining the working point (scan through cuts on network output)

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Construction of a test statistic:How to make 100 dimensions one real number…

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Neural Networks

Neural networks:Self learning procedures, copied from nature

ParietalCortexFrontal Lobe

Motor Cortex

Temporal Lobe

Brain Stem

OccipitalLobe

Cerebellum

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Neural Networks

The information(the knowledge, the expertise)is coded in the connectionsbetween the neurons

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Neural networks

Basis function

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Neural networks – transfer functions

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Neural networks - training

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

f t

Probability that hypothesisis correct (classification)or probability densityfor variable t

t

How it works: training and applicationHistoric or simulateddata

Data seta = ...b = ...c = .......t = …!

NeuroBayesNeuroBayes®®TeacherTeacher

NeuroBayesNeuroBayes®®ExpertExpert

Actual (new real) data

Data seta = ...b = ...c = .......t = ?

ExpertiseExpertise

Expert system

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Naïve networks and criticizmWe‘ve tried that but it didn‘t give good results

- Stuck in local minimum- Learning not robust

We‘ve tried that but it was worse than our 100 person-yearsanalytical high tech algorithm

- Selected too naive input variables- Use your fance algorithm as INPUT !

We‘ve tried that but the predictions were wrong- Overtraining: the net learnt statistical fluctuations

Yeah but how can you estimate systematic errors?- How can you with cuts when variables are correlated?

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Address all these topics and build a professional robust and flexible NeuralNetwork package for physics, insurance, bank and industry applications:NeuroBayes®

<phi-t>: Foundation out of University of Karlsruhe, sponsored by exist-seed-programme of thefederal ministery for Education and ResearchBMBF

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

2000-2002 NeuroBayes®-specialisationfor economy at the University of Karlsruhe

Oct. 2002: GmbH founded, first industrial projects

June 2003: Removal into new office199 qm IT-Portal Karlsruhe

Exclusive rights for NeuroBayes®

Personell currently4 full time staff (all from HEP) anda number of associated people,Prof. consultance z.B. by Prof. Dr. Volker Blobel,Economic/legal/marketing- expertise present

Customers: Badische Versicherungen, dm drogerie markt, Otto Versand

History

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

NeuroBayes® principle

NeuroBayes® Teacher:Learning of complex relationships from existingdata bases

NeuroBayes® Expert:Prognosis for unknown data

Output

Input

Sign

ific

ance

cont

rol

Postprocessing

Preprocessing

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Bayesian RegularisationUse Bayesian arguments to regularize network learning:

PosteriorPosterior EvidenceEvidence

LikelihoodLikelihood PriorPrior

Learn only statistically relevant information, suppress statistical noise

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Ramler-plot (extended correlation matrix)

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Ramler-II-plot (visualize correlation to target)

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Visualisation of single input-variables

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Visualisation of correlation matrix

Variable 1: Training target

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Visualisation of network performance

Purity vs. efficiency

Signal-effiziency vs. total efficiency(Lift chart)

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Visualisation of NeuroBayes network Topology

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Example DELPHI kaon ID ClassificationClassificationIdentification of kaons:

For Phi reconstruction:For Phi reconstruction:Efficiency twice as good Efficiency twice as good at the same background at the same background level (i.e. S/B doubled)level (i.e. S/B doubled)

Green: better of two Green: better of two competing standard competing standard algorithms (>50 men algorithms (>50 men years)years)

NeuroBayesNeuroBayes®®::Finds who is right under Finds who is right under which circumstanceswhich circumstances

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

NeuroBayes:Increase of efficiencyat same purity as best cut basedselection:Improve significancefrom 18.4 to 22.1

NeuroBayes:Increase of efficiencyat same purity as best cut basedselection:Improve significancefrom 18.4 to 22.1

Optimisation of Bs reconstruction for Bs oscillation analysisOptimisation of Bs reconstruction for Bs oscillation analysis

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Neural Nets for B flavour taggingNeural Nets for B flavour tagging

NeuroBayes track net:Does a track come from a B-decay or not?Tracknet 1 – Vertexnet – Tracknet 2

NeuroBayes track net:Does a track come from a B-decay or not?Tracknet 1 – Vertexnet – Tracknet 2

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Aim: Bayesian estimator for a singlemultidimensional measurement .

"Components of may be correlated."Components of should be correlated to t or its uncertainty. "All this should be learned automatically in a robust way from data bases"containing Monte-Carlo simulations or historical data.

Aim: Bayesian estimator for a singlemultidimensional measurement .

"Components of may be correlated."Components of should be correlated to t or its uncertainty. "All this should be learned automatically in a robust way from data bases"containing Monte-Carlo simulations or historical data.

Note: Conditional probability density contains much more information than just the mean value, which is determined in a regression analysis. It also tells us something about the uncertainty and the form of thedistribution, in particular non-Gaussian tails.

Note: Conditional probability density contains much more information than just the mean value, which is determined in a regression analysis. It also tells us something about the uncertainty and the form of thedistribution, in particular non-Gaussian tails.

xr

xr

xr

)|( xtfr

ConditionalConditional probabilityprobability densitydensity reconstructionreconstruction::

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Conditional probability densitiesin particle physics

What is the probability density of the true B energy in this event taken with the DELPHI detector at LEP IIat this beam energy, this effective c.m. energythese n tracks with those momenta and rapidities in the hemisphere, which are forming this secondary vertex with this decay length and probability, this number of not well reconstructed tracks, this neutral showers,etc pp )|( xtf

r

t

xr

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Conditional probability densitiesin investment bankingWhat is the probability density for a price change of equity A in the neyt 10 days…

that made this and that price movement in thelast days and weeks…

is so much more expensive than the n-days moving average…

but is so much less expensive that the absolute maximum…

has this correlation to the crude oil price…and the Dow Jones index…and etc. pp.

)|( xtfr

t

xr

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Prediction of the completeprobability distributionwith the < phi-t > NeuroBayes neural network

t

)|( xtfr

ModeExpectation value

Standard deviationvolatility

Deviations fromnormal distribution,e.g. crash probability

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Conditional probability densities f(t|x)

Conditional probability densities f(t|x) are functions of x, but also depend on marginal distribution f(t).

Conditional probability densities f(t|x) are functions of x, but also depend on marginal distribution f(t).

Inclusive distribution(Bayesian Prior)

Inclusive distribution(Bayesian Prior)

Conditional probability density for a special case x

(Bayesian Posterior)

Conditional probability density for a special case x

(Bayesian Posterior)

Marginal distribution f(t)Marginal distribution f(t)

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Classical ansatz:f(x|t)=f(t|x)

approximately correctat good resolution

far away fromphysical boundaries

Bayesian ansatz:takes into accounta priori- knowledge f(t):•Lifetime never negative•True lifetime exponentiallydistributed

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

No selection:Improved resolution

No selection:Improved resolution

NeuroBayes phi-direction

Best ”classical" chi**2- fit

(BSAURUS)

NeuroBayes phi-direction

Best ”classical" chi**2- fit

(BSAURUS)

Resolution of azimuthal angle of inclusively reconstructed B-hadrons in the DELPHI-

detector

first neural reconstruction of a direction

Resolution of azimuthal angle of inclusively reconstructed B-hadrons in the DELPHI-

detector

first neural reconstruction of a direction

Direction of B-mesons (DELPHI)

After selection cut on estimated error:Resolution massively improved, no tails

==> allows reliable selection of good events

After selection cut on estimated error:Resolution massively improved, no tails

==> allows reliable selection of good events

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Some applications in high energy physicsDELPHI:Kaon, proton, electron idOptimisation of resolutions inclusive B- E, phi, Theta, Q-valueB** enrichmentB fragmentation functionLimit on B_s-mixingB0-mixingB- F/B-asymmetryB-> wrong sign charmCDF: (Work in Progress)Electron ID, muon ID, kaon/proton IDOptimisation of resonance reconstruction (X, Y , B_s) Spin parity analysisB-Tagging for top, Higgs, etc. B-Flavour Tagging for mixing analyses

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Applications of NeuroBayes in Economy> Medicine and Pharma research

e.g. effects and undesirable effects of drugsearly tumor recognition

> Banks e.g. Credit-Scoring (Basel II), Finance time seriesprediction, valuation of derivates, risk minimisedtrading strategies, client valuation

> Insurancese.g. risk and cost prediction for individual clients, probability of contract cancellation, fraud recognition, justice in tariffs

> Trading chain stores: turnover prognosis for individual articles/stores

Necessary prerequisite:Historic or simulated data must be available!

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Risk analysis for a car insuranceBGV

Results for a the Badischen Gemeinde-Versicherungen:

since May 2003: radically new tariff for young drivers!

New variables added to calculation of the premium.Correlations taken into account.

Risk und premium up to a factor of 3 apart from each other!Even probability distribution of height of can be predicted

Premature contract cancellation also well predictable

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

The ‘‘unjustice‘‘ of insurance premiums

The majority of customers (with lowrisk) are paying too much.

Less than half of the customers (withlarger risk) do not pay enough, someby far not enough.These are currently subsidised by themore careful customers.

Anza

hl K

unde

n

Ratio of the accident risk calculated using NeuroBayes®to premium paid (normalised to same total premium sum):

Risiko/Prämie

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Prediction of contract cancellationfor an insurance

The predictionreally holds:

Test on a a newstatistic year

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Bank customers contract cancellation

Prognosis of prematurecontract cancellation

Massive enrichment possible.

CRM measures introduced

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Near Future TurnaroundPredictions for Chain Stores

1. Time series modelling2. Correction and error estimate

using NeuroBayes

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

The <phi-t> mouse game:or:

even your ``free will´´ is predictable

www.phi-t.de/mousegame

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Direct competition…Data-Mining-Cup 2005:Task: Internet shop: Prognosis of customerswho will not pay

531 Participantsfrom 176 Universitiesfrom 41 countries.

6 Karlsruhe studentsall using Phi-TNeuroBayes®:TOP RANKINGS: Positions 2,3,4,5,6,7!

www.data-mining-cup.de

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

How does NeuroBayes compare to other neural networks?How does NeuroBayes compare to other neural networks?

depends on problem.Usually superiorbecause of robustpreprocessing and Bayesian regularisation.

(does not meanthat Jetnet couldnot also do it ifpreprocessing isdone by hand)

depends on problem.Usually superiorbecause of robustpreprocessing and Bayesian regularisation.

(does not meanthat Jetnet couldnot also do it ifpreprocessing isdone by hand)Example: electron ID for CDF IIExample: electron ID for CDF II

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Hadron collider: No good MC for backgrounds availableMC for resonance production with different JPC assumptions

Idea: take background from sidebands in datacheck that network cannot learn mass

Hadron collider: No good MC for backgrounds availableMC for resonance production with different JPC assumptions

Idea: take background from sidebands in datacheck that network cannot learn mass

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

background-likehardly loose any signalbackground-likehardly loose any signal

signal-likesignal-like

X

soft NeuroBayesselection

X(3872) analysis:X(3872) analysis:

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Hard NeuroBayes cut:Very clean X(3872) signalHard NeuroBayes cut:Very clean X(3872) signal

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Training with weights:Neural Network Spin Parity AnalysisTraining with weights:Neural Network Spin Parity Analysis

Use data from sidebands as background sample

Use phase space decay MC with modelled pT distributionas signal sample

Calculate squared amplitudes for specific spin-parity assignmentsand use as weights in training

Hard cut on neural network trained by correct hypothesis shouldincrease signal over background

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Very hard NeuroBayes cuts:Very hard NeuroBayes cuts:

A good hypothesis for X A good hypothesis for X

JPC=1—(ππ)s hypothesisJPC=1—(ππ)s hypothesis

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Very hard NeuroBayes cuts:Very hard NeuroBayes cuts:

a not so good hypothesis for Xa not so good hypothesis for X

JPC=1—(ππ)s hypothesisJPC=1—(ππ)s hypothesis

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Hadron collider: Fast resonance S/N optimisation without MC:

Idea: Training with background subtractionSignal: Peak region weight 1

Sideband region with weight -1Background: Sideband region with weight 1

Hadron collider: Fast resonance S/N optimisation without MC:

Idea: Training with background subtractionSignal: Peak region weight 1

Sideband region with weight -1Background: Sideband region with weight 1

works very well!

also for Y(2S)and Y(3S) !Although just trained on Y(1S)

works very well!

also for Y(2S)and Y(3S) !Although just trained on Y(1S)

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Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

works very well also for Y(2S) and Y(3S) !Really learn to separate resonance from combinatorial backgroundworks very well also for Y(2S) and Y(3S) !Really learn to separate resonance from combinatorial background

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005

Making MC for hadronic background without specific model:Multidimensional correlated regression using NeuroBayesMaking MC for hadronic background without specific model:Multidimensional correlated regression using NeuroBayes

Use data in non-resonance region as signalUse phase space MC as background

Train NeuroBayes network,NN output O is Bayesian a posteriori probability that event stemsfrom signal (i.e. data distribution) rather than phase space MC:

O=P(S) with P(S)+P(B)=1Calculate weight W= P(S)/P(B) = O/(1-O) Phase space MC events with this weight W look like data!MC modelling of complicated background is possible!Opens new roads for likelihood fits

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Some kinematical variableDistributions(J/psi pi+pi- selection)

Black: real dataRed: weighted phase space MC

Physics with Neural Networks Michael Feindt Seminar Uni Freiburg Nov. 2005