Rare B meson decays - mathieu trocmé
Rare B meson decays - mathieu trocmé
Rare B meson decays - mathieu trocmé
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III- Analysis Method 37<br />
III.4- Optimisation of the cuts:<br />
III.4.1- Significance calculation:<br />
All the cuts values, except for ∆E and m ES , are optimised by maximising an<br />
approximation of the statistical significance of the branching ratio σ defined by:<br />
σ =<br />
s<br />
s + b<br />
where b is the number of background in the signal region (by analogy from above, it<br />
corresponds to nbg _ SR )<br />
b = R × ntot<br />
_ GSB<br />
and s is the estimated final number of events in the signal region (by analogy from above, it<br />
real<br />
corresponds to N sig )<br />
real '<br />
= N × BR × ε<br />
s 0<br />
B<br />
MC,<br />
corr<br />
(since still by analogy<br />
s × 1<br />
' ε<br />
BR = )<br />
N<br />
MC,<br />
corr<br />
real<br />
0<br />
B<br />
s is said estimated since the branching ratio BR’ used to calculate it must be assumed (for<br />
reason given later – Cf III.5, p.42) Although this may not completely reflect the true<br />
branching ratio for the channel under study, the optimisation is usually not heavily affected. A<br />
sensible value for it is usually the previous value found by someone else. The last person<br />
having studied this decay being N. Chevalier, the BR she found was used.<br />
Practically, each time a cut varies, 2 values change: the MC Efficiency appearing in s<br />
first, the number of events in the GSB leading to b secondly. Thus, by recalculating the<br />
corrected MC Efficiency and recounting the number of events in the GSB for each different<br />
value of one cut, the significance can be plotted versus these changing values and the<br />
maximum then found.