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THE CLs METHOD Statistica per l'analisi dei dati – Dottorato in Fisica – XXIX Ciclo Alessandro Pistone.

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Presentation on theme: "THE CLs METHOD Statistica per l'analisi dei dati – Dottorato in Fisica – XXIX Ciclo Alessandro Pistone."— Presentation transcript:

1 THE CLs METHOD Statistica per l'analisi dei dati – Dottorato in Fisica – XXIX Ciclo Alessandro Pistone

2 Introduction The ultimate goal of an experimental search for a new particle is to state whether or not a statistically significant observation of the signal has been made Is there a signal hidden in this data?

3 Statistical approach Define a test-statistic in order to separate
the signal+background hypothesis and the background-only hypothesis Compute from the observations the observed value of the test-statistic Decide to either fail to reject the null hypothesis or reject it in favor of an alternative hypothesis

4 Sensitive and insensitive experiments
CL s+b <0.05 with 1−CL b ≈0 CL s+b <0.05 with CL b ≈0 The experiment is not sensitive to the signal The experiment is sensitive to the signal Using this experiment to exclude the signal makes no sense!

5 The CLs method The modified frequentist confidence level CL s ≡ CL s+b CL b Normalizing CL s+b with CL b removes the dependence on background modelling: more conservative limits on signal+background hypothesis lower false exclusion rate than nominal 1−CL This presentation! A signal model is excluded at 95% confidence level if CL s <0.05

6 The model

7 The test-statistic: Likelihood-Ratio
Neyman-Pearson lemma most powerful test is the likelihood-ratio Q= L x|s+b L x|b with s b x L Q= i channels j bins s ij + b ij x ij e − s ij + b ij x ij ! b ij x ij e − b ij x ij ! −2ln Q = i channels j bins − s ij + x ij ln 1+ s ij b ij signal background data likelihood Expected to converge to χ s+b 2 − χ b 2 in the high-statistics limit

8 The Likelihood-Ratio distributions
Distributions evaluated running O 100k pseudo-experiments for different signal hypothesis

9 Coverage: p.d.f. mode Find Q ′ ⇔ CL s =0.05 and evaluate the corresponding CL s+b , then plot 1− CL s+b

10 Coverage: fit mode - i Find Q ′ ⇔ CL s =0.05 and Q ′′ ⇔ CL s+b =0.05 for different signal hypothesis 2nd generation of pseudo-experiments O 10k÷50k for different signal hypothesis Fit with theoretical distribution and evaluation of Q obs Exclusion if Q obs < Q ′ and Q obs < Q ′′

11 No sensible differences between χ 2 ≈1 and χ 2 ≈10
Coverage: fit mode - ii More sensible to fluctuations w/r/t the p.d.f. mode, robustness tested against: number of pseudo-experiments k sufficient seed of pseudo-random number generator ‰ on coverage errors used during the fit procedure No sensible differences between χ 2 ≈1 and χ 2 ≈10

12 Conclusion The correct behaviour of the coverage for the CL s method is reproduced


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