BAYES and FREQUENTISM: The Return of an Old Controversy 1 Louis Lyons Imperial College and Oxford University Heidelberg April 2013.

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Presentation transcript:

BAYES and FREQUENTISM: The Return of an Old Controversy 1 Louis Lyons Imperial College and Oxford University Heidelberg April 2013

2

Topics Who cares? What is probability? Bayesian approach Examples Frequentist approach Summary. Will discuss mainly in context of PARAMETER ESTIMATION. Also important for GOODNESS of FIT and HYPOTHESIS TESTING 3

4 It is possible to spend a lifetime analysing data without realising that there are two very different fundamental approaches to statistics: Bayesianism and Frequentism.

5 How can textbooks not even mention Bayes / Frequentism? For simplest case with no constraint onthen at some probability, for both Bayes and Frequentist (but different interpretations) See Bob Cousins “Why isn’t every physicist a Bayesian?” Amer Jrnl Phys 63(1995)398

6 We need to make a statement about Parameters, Given Data The basic difference between the two: Bayesian : Probability (parameter, given data) (an anathema to a Frequentist!) Frequentist : Probability (data, given parameter) (a likelihood function)

7 PROBABILITY MATHEMATICAL Formal Based on Axioms FREQUENTIST Ratio of frequencies as n  infinity Repeated “identical” trials Not applicable to single event or physical constant BAYESIAN Degree of belief Can be applied to single event or physical constant (even though these have unique truth) Varies from person to person *** Quantified by “fair bet”

8 Bayesian versus Classical Bayesian P(A and B) = P(A;B) x P(B) = P(B;A) x P(A) e.g. A = event contains t quark B = event contains W boson or A = I am in Heidelberg B = I am giving a lecture P(A;B) = P(B;A) x P(A) /P(B) Completely uncontroversial, provided….

9 Bayesian posteriorlikelihoodprior Problems: p(param) Has particular value “Degree of belief” Prior What functional form? Coverage Bayes’ Theorem p(param | data) α p(data | param) * p(param)

10 P(parameter) Has specific value “Degree of Belief” Credible interval Prior: What functional form? Uninformative prior: flat? In which variable? e.g. m, m 2, ln m,….? Even more problematic with more params Unimportant if “data overshadows prior” Important for limits Subjective or Objective prior?

11 Data overshadows prior Mass of Z boson (from LEP)

12 Prior Even more important for UPPER LIMITS

13 Prior = zero in unphysical region Mass-squared of neutrino

Bayes: Specific example Particle decays exponentially: dn/dt = (1/τ) exp(-t/τ) Observe 1 decay at time t 1 : L (τ) = (1/τ) exp(-t 1 /τ) Choose prior π(τ) for τ e.g. constant up to some large τ L Then posterior p(τ) = L (τ) * π(τ) has almost same shape as L (τ) Use p(τ) to choose interval for τ τ in usual way Contrast frequentist method for same situation later. 14

Bayesian posterior  intervals 15 Upper limit Lower limit Central interval Shortest

16 Ilya Narsky, FNAL CLW 2000 Upper Limits from Poisson data Upper Limits important for excluding models

17 P (Data;Theory) P (Theory;Data) HIGGS SEARCH at CERN Is data consistent with Standard Model? or with Standard Model + Higgs? End of Sept 2000: Data not very consistent with S.M. Prob (Data ; S.M.) < 1% valid frequentist statement Turned by the press into: Prob (S.M. ; Data) 99% i.e. “It is almost certain that the Higgs has been seen”

18 P (Data;Theory) P (Theory;Data)

19 P (Data;Theory) P (Theory;Data) Theory = male or female Data = pregnant or not pregnant P (pregnant ; female) ~ 3%

20 P (Data;Theory) P (Theory;Data) Theory = male or female Data = pregnant or not pregnant P (pregnant ; female) ~ 3% but P (female ; pregnant) >>>3%

21 Example 1 : Is coin fair ? Toss coin: 5 consecutive tails What is P(unbiased; data) ? i.e. p = ½ Depends on Prior(p) If village priest: prior ~ δ (p = 1/2 ) If stranger in pub: prior ~ 1 for 0 < p <1 (also needs cost function)

22 Example 2 : Particle Identification Try to separate π’s and protons probability (p tag; real p) = 0.95 probability ( π tag; real p) = 0.05 probability (p tag; real π ) = 0.10 probability ( π tag; real π ) = 0.90 Particle gives proton tag. What is it? If proton beam, very likely If general secondary particles, more even If pure π beam, ~ 0 Depends on prior = fraction of protons

Peasant and Dog 1)Dog d has 50% probability of being 100 m. of Peasant p 2)Peasant p has 50% probability of being within 100m of Dog d ? 23 dp x River x =0River x =1 km

24 Given that: a) Dog d has 50% probability of being 100 m. of Peasant, is it true that: b ) Peasant p has 50% probability of being within 100m of Dog d ? Additional information Rivers at zero & 1 km. Peasant cannot cross them. Dog can swim across river - Statement a) still true If dog at –101 m, Peasant cannot be within 100m of dog Statement b) untrue

25

26 Classical Approach Neyman “confidence interval” avoids pdf for Uses only P( x; ) Confidence interval : P( contains ) = True for any Varying intervals from ensemble of experiments fixed Gives range of for which observed value was “likely” ( ) Contrast Bayes : Degree of belief = is in

27 μ≥0 No prior for μ Classical (Neyman) Confidence Intervals Uses only P(data|theory)

Frequentism: Specific example Particle decays exponentially: dn/dt = (1/τ) exp(-t/τ) Observe 1 decay at time t 1 : L (τ) = (1/τ) exp(-t 1 /τ) Construct 68% central interval t =.17τ dn/dt τ t t = 1.8τ t 1 t 28 68% conf. int. for τ from t 1 /1.8  t 1 /0.17

Bob Cousins, “Why isn’t every physicist a Bayesian?” Amer Jrnl Phys 63(1995) Gaussian example Mass-squared of neutrino

Poisson, n=3 P n = e -µ µ n /n! 30 Frequentist Bayes and Likelihood

Poisson, n=3 P n = e -µ µ n /n! 31 Bayes. Prior =1/µ B and L

32 90% Classical interval for Gaussian σ = 1 μ ≥ 0 e.g. m 2 (ν e ), length of small object Other methods have different behaviour at negative x

33 at 90% confidence and known, but random unknown, but fixed Probability statement about and Frequentist Bayesian and known, and fixed unknown, and random Probability/credible statement about

Coverage Fraction of intervals containing true value Property of method, not of result Can vary with param Frequentist concept. Built in to Neyman construction Some Bayesians reject idea. Coverage not guaranteed Integer data (Poisson)  discontinuities Ideal coverage plot C μ 34

Coverage : L approach (Not frequentist) 35 P(n, μ) = e -μ μ n /n! (Joel Heinrich CDF note 6438) -2 lnλ< 1 λ = P(n,μ)/P(n,μ best ) UNDERCOVERS

Frequentist central intervals, NEVER undercovers (Conservative at both ends) 36

Feldman-Cousins Unified intervals Frequentist, so NEVER undercovers 37

Classical Intervals Problems 38 Hard to understand e.g. d’Agostini Arbitrary choice of interval Possibility of empty range Nuisance parameters (systematic errors ) Advantages Widely applicable Well defined coverage

FELDMAN - COUSINS Wants to avoid empty classical intervals  Uses “ L -ratio ordering principle” to resolve ambiguity about “which 90% region?”  [Neyman + Pearson say L -ratio is best for hypothesis testing] No ‘Flip-Flop’ problem 39

40 X obs = -2 now gives upper limit

41 Black lines Classical 90% central interval Red dashed: Classical 90% upper limit Flip-flop

42

43 Poisson confidence intervals. Background = 3 Standard Frequentist Feldman - Cousins

44

45

46 Importance of Ordering Rule Neyman construction in 1 parameter 2 measurements An aside: Determination of single parameter p via Acceptable level of Range of parameters given by 1)Values of for which data is likely i.e. p( ) is acceptable or 2) 2) is good 1) Range depends on [“Confidence interval coupled to goodness of fit”]

47 * * * Neyman Construction For given, acceptable (, ) satisfy = Defines cylinder in space Experiment gives interval Range depends on Range and goodness of fit are coupled

48 That was using Probability Ordering Now change to Likelihood Ratio Ordering For,no value of gives very good fit For Neyman Construction at fixed, compare: with where giving Cutting on Likelihood Ratio Ordering gives:

49 Therefore, range of is Constant Width Independent of Confidence Range and Goodness of Fit are completely decoupled

50 Standard Frequentist Pros: Coverage Widely applicable Cons: Hard to understand Small or empty intervals Difficult in many variables (e.g. systematics) Needs ensemble

51 Bayesian Pros: Easy to understand Physical interval Cons: Needs prior Coverage not guaranteed Hard to combine

52 Method: Mixed Frequentist - Bayesian Bayesian for nuisance parameters and Frequentist to extract range Philosophical/aesthetic problems? Highland and Cousins (Motivation was paradoxical behaviour of Poisson limit when LA not known exactly)

Basis of method Bayes Theorem  Posterior probability distribution Uses pdf for data, for fixed parameters Meaning of probability Degree of beliefFrequentist definition Prob of parameters? YesAnathema Needs prior?YesNo Choice of interval? YesYes (except F+C) Data considered Only data you have….+ other possible data Likelihood principle? YesNo 53 Bayesian versus Frequentism Bayesian Frequentist

Bayesian versus Frequentism Ensemble of experiment NoYes (but often not explicit) Final statement Posterior probability distribution Parameter values  Data is likely Unphysical/ empty ranges Excluded by priorCan occur SystematicsIntegrate over priorExtend dimensionality of frequentist construction CoverageUnimportantBuilt-in Decision making Yes (uses cost function)Not useful 54 Bayesian Frequentist

55 Bayesianism versus Frequentism “Bayesians address the question everyone is interested in, by using assumptions no-one believes” “Frequentists use impeccable logic to deal with an issue of no interest to anyone”

56 Next time: p-values, Upper Limits, Discoveries Hope: LHC moves us from era of ‘Upper Limits’ to that of even more DISCOVERIES