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Summary and Conclusions Kyle Cranmer (New York University)PowerPoint Presentation

Summary and Conclusions Kyle Cranmer (New York University)

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LPCC Workshop: Likelihoods for LHC Searches

Summary and Conclusions

Kyle Cranmer (New York University)

Harrison B. Prosper (Florida State University)

Sezen Sekmen (CERN)

LPCC Workshop on Likelihoods CERN

List of Talks

Day 1

- Sezen Goals
- Glen Principles
- Kyle Context/ScopeFeedback
- Marco
- Maggie
- Béranger

Day 2

- Kyle HistFactory
- Sven ATLAS HZZ4l
Higgs Combination

- Minshui CMS
- Haoshuang ATLAS
Day 3

- Wolfgang
- Javier (thanks Maurizio!)
- Wouter
PanelistsSünje, Mike, Lorenzo

LPCC Workshop on Likelihoods CERN

Day 1

LPCC Workshop on Likelihoods CERN

Sezen: Workshop Goals

Goals

- Educate ourselves: why are likelihoods needed?
- Move towards routine publication of likelihoods

LPCC Workshop on Likelihoods CERN

Glen: Basic Ideas

Distribution

Probability density (or mass) function, Nature(x)

x potential observations

Model

P(x| μ, θ) is a parametric model of the unknown function Nature(x) with parameters μ and θ, some of which are interesting (μ) and some not (θ).

Likelihood

L(μ, θ) = L(D | μ, θ) = P(D | μ, θ) D = observed data

LPCC Workshop on Likelihoods CERN

Glen: Basic Ideas

Need a way to get rid of parameters not of current interest. There are two general ways, marginalization and profiling:

Marginal Likelihood

Profile Likelihood

Profiling can be regarded as marginalization with the prior

LPCC Workshop on Likelihoods CERN

Kyle: Context & Scope

LPCC Workshop on Likelihoods CERN

Marco: Is it the SM Higgs?

LHC Higgs Cross Section Working Group

Assumptions

- SM tensor structure (CP-even scalar)
- A single zero-width resonance
- κi = σi / σSMi and κf = Γf / ΓSMi are free parameters, where
How do we best report experimental results

(with the goal of allowing more

detailed/accurate studies)?

LPCC Workshop on Likelihoods CERN

Maggie: Is it the SM Higgs?

Can use an effective field theory (EFT) approach:

LPCC Workshop on Likelihoods CERN

Maggie: Is it the SM Higgs?

LPCC Workshop on Likelihoods CERN

Béranger: Is it the SM Higgs?

Effective Lagrangian

Fitting procedure

LPCC Workshop on Likelihoods CERN

Béranger: Is it the SM Higgs?

LPCC Workshop on Likelihoods CERN

Day 2

LPCC Workshop on Likelihoods CERN

Kyle: HistFactory

Equivalent to a multi-bin Poisson model with bins so small that the chance of > a single count per bin is negligible

n is the number of events and {xe} are the measurements (e.g., the di-photon masses)

In general, f is a mixture:

LPCC Workshop on Likelihoods CERN

Kyle: HistFactory

which, in this case, represents a Gaussian G(x| μ, σ).

fp(ap | αp) are the likelihoods of the auxiliary measurements ap from either real, simulated, or hypothetical experiments.

These functions provide constraints on the parameters α and hence on the parameters νc(α).

LPCC Workshop on Likelihoods CERN

Kyle: HistFactory

XML representation of model

Kyle

RooWorkspace

HistFactory

http://www.brianlemay.com/

LPCC Workshop on Likelihoods CERN

Sven: HZZ*(4l) in ATLAS

LPCC Workshop on Likelihoods CERN

Sven: HZZ*(4l) in ATLAS

Kernel density estimation

+ density morphing

+ HistFactory

Cranmer, K,

Kernel Estimation in High-Energy Physics

Computer Physics Communications

136:198-207, 2001

hep ex/0011057

LPCC Workshop on Likelihoods CERN

Sven: HZZ*(4l) in ATLAS

Editorial comment: Jack’s intuition is spot on! For discrepant

results, the combined result ought to be worse.

LPCC Workshop on Likelihoods CERN

Sven: HZZ*(4l) in ATLAS

Clarity Prize goes to Sven for explaining to me why a p-value computed from the background-only hypothesis depends on the alternative hypothesis!

Harrison: “Please explain this plot”

Sven: “The sampling distribution

of t(x) = -2 lnLp/Lmax is independent

of mH, as it should be, but the power

of the test is maximized for eachmH,

so the observed value of t

changes with mH”

LPCC Workshop on Likelihoods CERN

Mingshui: Higgs Combination (CMS)

Model: Marked Poisson Process (see Kyle’s HistFactory talk)

LEP

No constraints for parameters θ with systematic uncertainties

Tevatron

Use priors π(θ|θ0) to constrain θ

LHC

Interpret π(θ|θ0) as π(θ|θ0) ~ f(θ0|θ) π(θ)

Cowanscher Ur-prior!

and interpret f(θ0|θ) as the likelihood for auxiliary measurements θ0

LPCC Workshop on Likelihoods CERN

Mingshui: Higgs Combination (CMS)

Assumptions (current measurements)

- Data are disjoint
- Standard Model with mH and μ as free parameters
- Same mH for all channels
Detailed models can be provided in RooWorkspace form

LPCC Workshop on Likelihoods CERN

Haoshuang: Higgs Combination (ATLAS)

Basic tool is HistFactory for all channels except for H to γγ

A Single Channel

LPCC Workshop on Likelihoods CERN

Haoshuang: Higgs Combination (ATLAS)

Important point

In combining channels the Greek symbol fallacy is avoided. An explicit decision must be made about how parameters with the same name are related, if at all.

Typically done by modifying the XML representation of the model.

LPCC Workshop on Likelihoods CERN

Day 3

LPCC Workshop on Likelihoods CERN

Wolfgang: BSM Searches

Guided by a well-motivated theory, e.g., the pMSSM, and its simplified model decomposition

pMSSM Results (non-CMS)

…but CMS pMSSM / SMs analysis in progress…

LPCC Workshop on Likelihoods CERN

Wolfgang: BSM Searches

LPCC Workshop on Likelihoods CERN

Javier: BSM Searches

LPCC Workshop on Likelihoods CERN

Javier: BSM Searches

LPCC Workshop on Likelihoods CERN

Javier: BSM Searches

LPCC Workshop on Likelihoods CERN

Javier: BSM Searches

Nuisance parameters

marginalized through

Monte Carlo integration

LPCC Workshop on Likelihoods CERN

Wouter: RooFit

RooFit is a probability modeling language:

RooStats provides high level statistical tools that use RooFit models

LPCC Workshop on Likelihoods CERN

Wouter: RooFit

ARooWorkspace is a mechanism to store a model + data

LPCC Workshop on Likelihoods CERN

Panel Discussion

Sünje, Mike, Lorenzo

HEPData on INSPIRE

Make data sets searchable, findable, citable

Assign Digital Object Identifier (DOI) to data

- Should we track the re-use of data?
- Should we have a single portal (e.g, Inspire)?
- Will will have a single portal?
- Will need non-web access also
- RECAST requests that are honored could yield citation
- Are there legal issues?

LPCC Workshop on Likelihoods CERN

Conclusions

LPCC Workshop on Likelihoods CERN

ICHEP 2040

The New Standard Model has been firmly established

pNMSSM

me, mμ, mτ

mu, md, ms, mc, mb, mt

θ12, θ23, θ13, δ

g1, g2, g3

θQCD

μ, λ

SM

OTTRTA

Data

LPCC Workshop on Likelihoods CERN

Conclusions

We could do a better job of understanding the LHC data if more information were made public in a systematic way

A general way to do this is to publish the probability model + relevant data set

The technology exists (RooWorkspace, Inspire, HepData) to publish arbitrarily complicated models, retrieve them and use them in analyses

My sense is that our field is nearing a tipping point, for the better!

LPCC Workshop on Likelihoods CERN

Thanks!

- We thank the LHC Physics Centre at CERN (LPCC) for hosting this workshop and its financial support of two RooStats developers. We thank the Theory Secretariat for organizing the coffee breaks!
- We thank YOU for making this workshop both informative and enjoyable.
- We thank the World’s funding agencies and the World’s taxpayers for their generous support:
LHC cost: $1million / scientist

LPCC Workshop on Likelihoods CERN

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