Direct Maximum Likelihood Methods David Szwer Hannes Busche; Dan Maxwell; David Paredes; Charles Adams; Matt Jones Group meeting 12/03/2012 Talk Overview • Uncertainty in Arcsine • Introduction to Maximum Likelihood • Maximum Likelihood for Arcsine Arcsine • Measure r ± αr . • Calculate θ = asin(r); what is αθ? Arcsine • θ = asin(r). Arcsine • Measure r ± αr . • Calculate θ = asin(r); what is αθ? • Calculus method: r r r 1 r 2 Arcsine, Derivative Method • θ = asin(r). • αθ → ∞ as r → ±1. Arcsine, Functional Method • θ = asin(r). • θ+αθ = asin(r+αr) θ–αθ = asin(r–αr). Arcsine, Functional Method • When r ≈±1, only one of the errors is well defined. Arcsine, Functional Method • When |r |>1, θ can’t be calculated. Must we just throw away that data? Introduction to Maximum Likelihood • “Likelihood” is probability of Data given Hypothesis and background Information L = P(D|H,I) • Used to derive χ2 least-squares fitting. – Least-squares fitting adjusts parameters of H to maximise L. Notation from Toussaint, “Bayesian Inference in Physics”, Rev. Mod. Phys. 83 943-999 (2011) Introduction to Maximum Likelihood • “Likelihood” is probability of Data given Hypothesis and background Information L = P(D|H,I) • Used to derive χ2 least-squares fitting. – Least-squares fitting adjusts parameters of H to maximise L. Notation from Toussaint, “Bayesian Inference in Physics”, Rev. Mod. Phys. 83 943-999 (2011) Arcsine, Maximum Likelihood L = P(D|H,I) • Data D is just “r”. Arcsine, Maximum Likelihood L = P(D|H,I) • Data D is just “r”. • Hypothesis H is “θtrue=θ0”. Arcsine, Maximum Likelihood L = P(D|H,I) • Data D is just “r”. • Hypothesis H is “θtrue=θ0”. • Assumptions I include “Uncertainty in r is Gaussian” and “θ = asin(r)”. Arcsine, Maximum Likelihood L = P(D|H,I) • Data D is just “r”. • Hypothesis H is “θtrue=θ0”. • Assumptions I include “Uncertainty in r is Gaussian” and “θ = asin(r)”. 1 L( r | 0 ) e 2 r asin r 0 12 r 2 Arcsine, Maximum Likelihood • L = P(D|H,I) = P(r|θ0) Arcsine, Maximum Likelihood • Bayes’ Theorem PH | I PD | H , I PH | D, I PD | I Arcsine, Maximum Likelihood • Bayes’ Theorem PH | I PD | H , I PH | D, I PD | I • Posterior: P(H|D,I) = P(θ0|r) Arcsine, Maximum Likelihood • Bayes’ Theorem PH | I PD | H , I PH | D, I PD | I • Posterior: P(H|D,I) = P(θ0|r) • Likelihood: L = P(D|H,I) = P(r|θ0) Arcsine, Maximum Likelihood • Bayes’ Theorem PH | I PD | H , I PH | D, I PD | I • Posterior: P(H|D,I) = P(θ0|r) • Likelihood: L = P(D|H,I) = P(r|θ0) • Prior: P(H|I) = P(θ0) – Assume uniform prior –π/2 ≤ θ0 < π/2. Arcsine, Maximum Likelihood • Bayes’ Theorem PH | I PD | H , I PH | D, I PD | I • Posterior: P(H|D,I) = P(θ0|r) • Likelihood: L = P(D|H,I) = P(r|θ0) • Prior: P(H|I) = P(θ0) – Assume uniform prior –π/2 ≤ θ0 < π/2. • Evidence: P(D|I) = P(r) – Normalisation constant • P(θ0|r)QP(r|θ0) for fixed r. Arcsine, Maximum Likelihood • L = P(D|H,I) = P(r|θ0) Arcsine, Maximum Likelihood • Renormalize for r. • P(H|D,I) = P(θ0|r) Arcsine, Maximum Likelihood • Small |r|: approximately Gaussian. Arcsine, Maximum Likelihood • Distorted for larger |r|. Arcsine, Maximum Likelihood • r=±1 handled easily... Arcsine, Maximum Likelihood • Renormalize for r. • P(H|D,I) = P(θ0|r) Arcsine, Maximum Likelihood • ...as is |r|>1: gives θ0=±π/2 and sensible uncertainty. Arcsine, Summary Arcsine, Summary Arcsine, Summary • Max. likelihood error estimated as 2 P 0 | r 0 asin r d 0 2 2 2 Cons • Direct maximum likelihood: • Does not give single uncertainty figure. – Does not “plug-in” to other frequentist methods. • Computation-intensive. Cons and Pros • Direct maximum likelihood: • Does not give single uncertainty figure. – Does not “plug-in” to other frequentist methods. • Computation-intensive. • Works for badlybehaved functions. • Gives full Posterior distribution. • Extends easily to nonuniform priors via Bayes’ theorem. References • Hughes and Hase, “Measurements and their Uncertainties”, OUP (2010) • Toussaint, “Bayesian Inference in Physics”, Rev. Mod. Phys. 83 943-999 (2011) • MacKay, “Information Theory, Inference and Learning Algorithms”, CUP (2003). Available online: http://www.inference.phy.cam.ac.uk/mackay /itila/ – See especially sections 3.1, 22.1 and 24.1.
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