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Transcript
Statistical Methods in Particle Physics
(Di
(Discovery and Exclusion)
dE l i )
SSaeid Paktinat
id P k i
IPM
IPM National School on the Phenomenological And Experimental aspects of the Elementary Particle Physics
16‐19 Oct 2007
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
1
5 sigma significance
5‐sigma significance
• Imagine there is a theory that pdf of the p p
people’s height is Gaussian with mean 165cm g
and RMS 15cm.
• There is somebody as high as 200 cm, is There is somebody as high as 200 cm is
theory violated? What about a man with 280 cm?
• How to quantify this violation.
How to quantify this violation.
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
2
Some conventions
Some conventions
• A theory is considered to be close to violation if something happens with a probability less than 10‐3
(3‐sigma)
• A theory is excluded if something happens with a probability less than 10‐7 (5‐sigma)
p=∫
+∞
x
19 Oct 2007
f ( x)dx
Statistical Methods in Particle Physics S.Paktinat
3
An example from hep
An example from hep
• SM without higgs predicts that after a set of cuts 64 events will remain, but in reality 80 events are found, is it the higgs signal?
• No, because 80‐64 = 16 = 2 * sqrt(64)
• Remember that RMS for a poisson distribution is sq ( ea )
sqrt(mean)
significance =
19 Oct 2007
N observed − N ppredicted
σ N predicted
Statistical Methods in Particle Physics S.Paktinat
4
Significance(s)?!
S
S1 =
B
S2 =
•Statistical uncertainty ONLY!
S
S+B
50% di
50% discovery probability
b bilit
S 12 = 2 ( S + B −
19 Oct 2007
B)
Statistical Methods in Particle Physics S.Paktinat
5
More formal
More formal
• nb is predicted by SM, if nb is large, probability to observe nobs is:
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
6
Another example from hep
Another example from hep
• HÆγγ
Æ (m
( H = 110 GeV/c
/ 2) @ CMS )
with IL = 30 (20) fb‐1
• S = 357 (238), B = 2893 (1929)
• S1 1 = 6.6 (5.4)
6 6 (5 4)
• It means that CMS can achieve 5σ discovery for H (110 GeV) with the probability of 93(60)%.
CMS CR 2002/05
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
7
Confidence Interval
Confidence Interval
• A quantity X is measured with error σ, the result is used as the estimator of the real value. x ±σ
or even
+σ+
x
−σ−
• It does not mean that It does not mean that P( x − σ − < X < x + σ + ) = 0.68
• ( x − σ − , x + σ + ) is the 68% confidence interval for X.
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
8
Confidence Interval
Confidence Interval
• Or if the same method is repeated 100 times in 68 times X will lie inside the confidence intervals.
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
9
Confidence Interval
Confidence Interval
• In an experiment B +/‐ σΒ events from SM is p
expected. N events are observed:
|N ‐ B| < 1.64 (1.96) * σΒ means that SM agrees at 90(95)% C L with the experiment
agrees at 90(95)% C.L. with the experiment.
|N ‐ B| > 5 * σΒ means that SM is excluded, P(N;B, σΒ) < 10‐7
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
10
Confidence Interval
Confidence Interval
• A model with a new physics predicts S+B+/‐
/ σS+B;; N events are observed:
|N – S ‐ B| < 1.64 (1.96) * σS+B means that the model with a new physics agrees
model with a new physics agrees
90(95)% C.L. with the experiment.
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
11
Exclusion
• If |N ‐ B| < 1.64 (1.96) * σΒ (SM agrees at ( )
p
)
90(95)% C.L. with the experiment.) Some exclusion limit on new physics (limit on S) can be obtained by solving:
be obtained by solving:
|N – S ‐ B| < 1.96 * σS+B
An example: N = B = 100, σS+B = sqrt(S+B)
S < 22 at 95% C L
S < 22 at 95% C.L.
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
12
Back up
Back up
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
13
Famuos pdf’s (Gaussian pdf)
When many small, independent effects are y
g
additively contributing to each observation the result follows the Gaussian (normal) distribution e.g,
distribution, e g people
people’ss height.
height
⎛ ((x − μ)2 ⎞
1
⎟⎟
f( ; μ , σ) =
f(x
exp⎜⎜ −
2
2σ ⎠
σ 2π
⎝
19 Oct 2007
Statistical Methods in Particle Physics S.Paktinat
14