G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 1 Minimum Power for PCL ATLAS Statistics Forum EVO, 10 June, 2011 Glen Cowan* Physics Department.

Slides:



Advertisements
Similar presentations
Hypothesis testing Another judgment method of sampling data.
Advertisements

Anthony Greene1 Simple Hypothesis Testing Detecting Statistical Differences In The Simplest Case:  and  are both known I The Logic of Hypothesis Testing:
Using the Profile Likelihood in Searches for New Physics / PHYSTAT 2011 G. Cowan 1 Using the Profile Likelihood in Searches for New Physics arXiv:
G. Cowan Statistics for HEP / LAL Orsay, 3-5 January 2012 / Lecture 3 1 Statistical Methods for Particle Physics Lecture 3: More on discovery and limits.
G. Cowan RHUL Physics Profile likelihood for systematic uncertainties page 1 Use of profile likelihood to determine systematic uncertainties ATLAS Top.
Introduction to Hypothesis Testing
Hypothesis Testing: Type II Error and Power.
Lecture 2: Thu, Jan 16 Hypothesis Testing – Introduction (Ch 11)
G. Cowan Statistical methods for HEP / Freiburg June 2011 / Lecture 3 1 Statistical Methods for Discovery and Limits in HEP Experiments Day 3: Exclusion.
G. Cowan RHUL Physics Comment on use of LR for limits page 1 Comment on definition of likelihood ratio for limits ATLAS Statistics Forum CERN, 2 September,
G. Cowan Statistical methods for HEP / Birmingham 9 Nov Recent developments in statistical methods for particle physics Particle Physics Seminar.
G. Cowan Lectures on Statistical Data Analysis Lecture 12 page 1 Statistical Data Analysis: Lecture 12 1Probability, Bayes’ theorem 2Random variables and.
G. Cowan 2011 CERN Summer Student Lectures on Statistics / Lecture 41 Introduction to Statistics − Day 4 Lecture 1 Probability Random variables, probability.
G. Cowan RHUL Physics Higgs combination note status page 1 Status of Higgs Combination Note ATLAS Statistics/Higgs Meeting Phone, 7 April, 2008 Glen Cowan.
BCOR 1020 Business Statistics Lecture 21 – April 8, 2008.
G. Cowan Statistics for HEP / NIKHEF, December 2011 / Lecture 2 1 Statistical Methods for Particle Physics Lecture 2: Tests based on likelihood ratios.
G. Cowan Statistical Data Analysis / Stat 4 1 Statistical Data Analysis Stat 4: confidence intervals, limits, discovery London Postgraduate Lectures on.
G. Cowan Shandong seminar / 1 September Some Developments in Statistical Methods for Particle Physics Particle Physics Seminar Shandong University.
G. Cowan Discovery and limits / DESY, 4-7 October 2011 / Lecture 2 1 Statistical Methods for Discovery and Limits Lecture 2: Tests based on likelihood.
Business Statistics: A Decision-Making Approach, 6e © 2005 Prentice-Hall, Inc. Chap 8-1 TUTORIAL 6 Chapter 10 Hypothesis Testing.
G. Cowan Lectures on Statistical Data Analysis 1 Statistical Data Analysis: Lecture 7 1Probability, Bayes’ theorem, random variables, pdfs 2Functions of.
G. Cowan Discovery and limits / DESY, 4-7 October 2011 / Lecture 3 1 Statistical Methods for Discovery and Limits Lecture 3: Limits for Poisson mean: Bayesian.
G. Cowan RHUL Physics Bayesian Higgs combination page 1 Bayesian Higgs combination using shapes ATLAS Statistics Meeting CERN, 19 December, 2007 Glen Cowan.
G. Cowan Statistics for HEP / NIKHEF, December 2011 / Lecture 4 1 Statistical Methods for Particle Physics Lecture 4: More on discovery and limits.
1 In the previous sequence, we were performing what are described as two-sided t tests. These are appropriate when we have no information about the alternative.
Copyright © 2005 Brooks/Cole, a division of Thomson Learning, Inc Chapter 11 Introduction to Hypothesis Testing.
1 © Lecture note 3 Hypothesis Testing MAKE HYPOTHESIS ©
1 Dr. Jerrell T. Stracener EMIS 7370 STAT 5340 Probability and Statistics for Scientists and Engineers Department of Engineering Management, Information.
Chapter 20: Testing Hypotheses about Proportions
Business Statistics: A Decision-Making Approach, 6e © 2005 Prentice-Hall, Inc. Chap th Lesson Introduction to Hypothesis Testing.
Chapter 9 Hypothesis Testing: Single Population
Inference for a Single Population Proportion (p).
Psy B07 Chapter 4Slide 1 SAMPLING DISTRIBUTIONS AND HYPOTHESIS TESTING.
1 Lecture note 4 Hypothesis Testing Significant Difference ©
Statistics In HEP Helge VossHadron Collider Physics Summer School June 8-17, 2011― Statistics in HEP 1 How do we understand/interpret our measurements.
G. Cowan Statistical techniques for systematics page 1 Statistical techniques for incorporating systematic/theory uncertainties Theory/Experiment Interplay.
Chap 8-1 A Course In Business Statistics, 4th © 2006 Prentice-Hall, Inc. A Course In Business Statistics 4 th Edition Chapter 8 Introduction to Hypothesis.
Economics 173 Business Statistics Lecture 4 Fall, 2001 Professor J. Petry
Copyright ©2013 Pearson Education, Inc. publishing as Prentice Hall 9-1 σ σ.
ROOT and statistics tutorial Exercise: Discover the Higgs, part 2 Attilio Andreazza Università di Milano and INFN Caterina Doglioni Université de Genève.
G. Cowan RHUL Physics page 1 Status of search procedures for ATLAS ATLAS-CMS Joint Statistics Meeting CERN, 15 October, 2009 Glen Cowan Physics Department.
G. Cowan, RHUL Physics Discussion on significance page 1 Discussion on significance ATLAS Statistics Forum CERN/Phone, 2 December, 2009 Glen Cowan Physics.
G. Cowan RHUL Physics LR test to determine number of parameters page 1 Likelihood ratio test to determine best number of parameters ATLAS Statistics Forum.
G. Cowan CERN Academic Training 2010 / Statistics for the LHC / Lecture 41 Statistics for the LHC Lecture 4: Bayesian methods and further topics Academic.
Inferential Statistics Inferential statistics allow us to infer the characteristic(s) of a population from sample data Slightly different terms and symbols.
G. Cowan Report from the Statistics Forum / CERN, 23 June Report from the Statistics Forum ATLAS Week Physics Plenary CERN, 23 June, 2011 Glen Cowan,
G. Cowan RHUL Physics Input from Statistics Forum for Exotics page 1 Input from Statistics Forum for Exotics ATLAS Exotics Meeting CERN/phone, 22 January,
Easy Limit Statistics Andreas Hoecker CAT Physics, Mar 25, 2011.
G. Cowan Lectures on Statistical Data Analysis Lecture 8 page 1 Statistical Data Analysis: Lecture 8 1Probability, Bayes’ theorem 2Random variables and.
G. Cowan Lectures on Statistical Data Analysis Lecture 4 page 1 Lecture 4 1 Probability (90 min.) Definition, Bayes’ theorem, probability densities and.
G. Cowan Statistical methods for particle physics / Cambridge Recent developments in statistical methods for particle physics HEP Phenomenology.
G. Cowan Computing and Statistical Data Analysis / Stat 9 1 Computing and Statistical Data Analysis Stat 9: Parameter Estimation, Limits London Postgraduate.
G. Cowan RHUL Physics Analysis Strategies Workshop -- Statistics Forum Report page 1 Report from the Statistics Forum ATLAS Analysis Strategies Workshop.
G. Cowan, RHUL Physics Statistics for early physics page 1 Statistics jump-start for early physics ATLAS Statistics Forum EVO/Phone, 4 May, 2010 Glen Cowan.
G. Cowan Statistical methods for particle physics / Wuppertal Recent developments in statistical methods for particle physics Particle Physics.
G. Cowan RHUL Physics Status of Higgs combination page 1 Status of Higgs Combination ATLAS Higgs Meeting CERN/phone, 7 November, 2008 Glen Cowan, RHUL.
G. Cowan Lectures on Statistical Data Analysis Lecture 12 page 1 Statistical Data Analysis: Lecture 12 1Probability, Bayes’ theorem 2Random variables and.
G. Cowan Statistical methods for HEP / Freiburg June 2011 / Lecture 2 1 Statistical Methods for Discovery and Limits in HEP Experiments Day 2: Discovery.
Lec. 19 – Hypothesis Testing: The Null and Types of Error.
Statistical Inference for the Mean Objectives: (Chapter 8&9, DeCoursey) -To understand the terms variance and standard error of a sample mean, Null Hypothesis,
G. Cowan RHUL Physics Statistical Issues for Higgs Search page 1 Statistical Issues for Higgs Search ATLAS Statistics Forum CERN, 16 April, 2007 Glen Cowan.
G. Cowan SLAC Statistics Meeting / 4-6 June 2012 / Two Developments 1 Two developments in discovery tests: use of weighted Monte Carlo events and an improved.
G. Cowan CERN Academic Training 2012 / Statistics for HEP / Lecture 21 Statistics for HEP Lecture 2: Discovery and Limits Academic Training Lectures CERN,
Inference for a Single Population Proportion (p)
Discussion on significance
Statistics for the LHC Lecture 3: Setting limits
TAE 2018 / Statistics Lecture 3
Hypothesis Testing A hypothesis is a claim or statement about the value of either a single population parameter or about the values of several population.
Decomposition of Stat/Sys Errors
Presentation transcript:

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 1 Minimum Power for PCL ATLAS Statistics Forum EVO, 10 June, 2011 Glen Cowan* Physics Department Royal Holloway, University of London * with Kyle Cranmer, Eilam Gross, Ofer Vitells

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 2 Outline Quick review of Power-Constrained Limits For more details see: G. Cowan, K. Cranmer, E. Gross and O. Vitells, Power-Constrained Limits, arXiv: Choice of minimum power threshold: rationale for 16% rationale for 50%

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 3 Review of Power-Constrained Limits The basic idea is to consider a parameter value μ as excluded if two criteria are satisfied: (a) The value μ is rejected by a statistical test, e.g., the p-value of μ is found less than a = 5%. The highest value not excluded is the unconstrained limit, μ up. (b) The sensitivity to μ exceeds a specified threshold. The measure of sensitivity is the power M 0 (μ) of the test of μ with respect to the alternative μ = 0, i.e., the probability to reject μ if μ = 0 is true. I.e. require M 0 (μ) ≥ M min for some appropriately chosen power threshold M min. The highest value not excluded by both (a) and (b) is the power-constrained limit, μ* up.

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 4 Illustration of low/high sensitivity Power M 0 (μ) is the area under the dashed curve in the critical region.

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 5 Choice of minimum power Choice of M min is convention; earlier we have proposed because in Gaussian example this means that one applies the power constraint if the observed limit fluctuates down by one standard deviation. In fact the distribution of μ up is often roughly Gaussian, so we call this a “1σ” (downward) fluctuation and use M min = 0.16 regardless of the exact distribution of μ up. For the Gaussian example, this gives μ min = 0.64σ. This is reasonable – the lowest limit is of the same order as the intrinsic resolution of the measurement (σ).

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 6 PCL and CLs/Bayesian for x ~ Gauss(μ, σ)

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 7 PCL as a function of, e.g., m H PCL Here power below threshold; do not exclude.

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 8 Some reasons to consider increasing M min M min is supposed to be “substantially” greater than α (5%). So M min = 16% is fine for 1 – α = 95%, but if we ever want 1 – α = 90%, then16% is not “large” compared to 10%; μ min = 0.28σ starts to look small relative to the intrinsic resolution of the measurement. Not an issue if we stick to 95% CL. PCL with M min = 16% is often substantially lower than CLs. This is because of the conservatism of CLs (see coverage). But goal is not to get a lower limit per se, rather (a)to use a test with higher power in those regions where one feels there is enough sensitivity to justify exclusion and (b) to allow for easy communication of coverage (95% for μ ≥ μ min ; 100% otherwise).

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 9 PCL with M min = 0.16, 0.50 (and other limits) With M min = 50%, power constraint is applied half the time. This is somewhat contrary to the original spirit of preventing a “lucky” fluctuation from leading to a limit that is small compared to the intrinsic resolution of the measurement. But PCL still lower than CLs most of the time (e.g., x >  0.4).

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 10 Aggressive conservatism It could be that owing to practical constraints, certain systematic uncertainties are over-estimated in an analysis; this could be justified by wanting to be conservative. The consequence of this will be that the +/-1 sigma bands of the unconstrained limit are broader than they otherwise would be. If the unconstrained limit fluctuates low, it could be that the PCL limit, constrained at the -1sigma band, is lower than it would be had the systematics been estimated correctly. conservative = aggressive If the power constraint M min is at 50%, then by inflating the systematics the median of the unconstrained limit is expected to move less (or not at all).

G. Cowan ATLAS Statistics Forum / Minimum Power for PCL 11 A few further considerations Obtaining PCL requires the distribution of unconstrained limits, from which one finds the M min (16%, 50%) percentile. In some analyses this can entail calculational issues that are expected to be less problematic for M min = 50% than for 16%. Analysts produce anyway the median limit, even in absence of the error bands, so with M min = 50% the burden on the analyst is reduced somewhat (but one would still want the error bands). Changing M min now may be too short notice for EPS, or, one may argue that if we are going to make the change, now is the time. We propose moving M min to 50% and to report both PCL and CLs. We propose using PCL as the primary result.