Decomposition of Stat/Sys Errors

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Decomposition of Stat/Sys Errors ATLAS Statistics Forum CERN, 12 September 2017 Glen Cowan Physics Department Royal Holloway, University of London www.pp.rhul.ac.uk/~cowan g.cowan@rhul.ac.uk G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors Background info Recall prototypical analysis: primary data x, parameter of interest μ, nuisance parameter(s) θ = (θ1,..., θΝ), control measurements y, model P(x, y | μ, θ) = L(μ, θ) (the likelihood). Often control measurements are designed to constrain a particular nuisance parameter, e.g., yi = θi, could be “best guess” of θi, but treated as a measurement with a sampling distribution p(θi|θi). ~ ~ ^ Maximize the likelihood → μ Variance of μ reflects total uncertainty, i.e., the model with nuisance parameters is “correct”, no systematic uncertainty. ^ G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors Commonly used method 1) Identify source of systematic with nuisance parameter θ. 2) Fix θ = θ0 3) Repeat fit, get μθ0 4) Get variance V[μθ0] 5) σsys,θ = (V[μ] – V[μθ0])1/2 But what about nuisance parameters that we expect to be (at least partially) constrained by the data, e.g, background level/shape? At least some portion of the uncertainty in such nuisance parameters is more logically regarded as a statistical error. ^ ^ ^ ^ G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

Alternative approach / example Goal (?) of stat/sys breakdown is to communicate how the uncertainty is expected to scale with luminosity, so, define ratio of lumi to that of actual measurement and rewrite model so as to include lambda. E.g., Here μ is parameter of interest (~signal rate); β (~background rate) and θ (scale factor) are nuisance parameters. x is “main” measurement; y and z are control measurements. G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors Example (2) Likelihood = product of 3 Gaussians → -2ln L gives Minimizing χ2 gives estimators Linear error propagation gives the variance stat sys G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

Result of example (constant σz) Plot variance versus λ-1, intercept at zero (infinite lumi) corresponds to systematic error: G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors Variation on example But suppose the std. deviation of control measurement z had been modeled as Here σz0 will contribute to the part that does not change with λ, (systematic error), σz1 to part that goes as 1/λ (stat error). But in the first (“commonly used”) method, fixing θ would in in effect treat both as part of the systematic uncertainty. G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

MC (exact) determination of variance Estimator for μ nonlinear in z, so error propagation not exact; use MC to get variance: G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors

ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors Extrapolate or not? Behaviour in region near nominal lumi may seem like reasonable basis for stat/sys decomposition, but may not give meaningful extrapolation to infinite lumi: G. Cowan ATLAS Stat Forum 12 Sep 2017 / Decomposition of Stat/Sys Errors