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Violation in Mixing

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7.4 Data samples and event selection 171<br />

Figure 7-2. The fitted �� yield divided by its error for three samples of 1000 toy experiments correspond<strong>in</strong>g<br />

to different cuts on Ó× �Ë.<br />

The separation between signal and background <strong>in</strong> the Fisher variable is reduced when cutt<strong>in</strong>g harder on<br />

� Ó× �Ë�, which partially compensates the <strong>in</strong>creased signal-to-background ratio. To optimize this cut,<br />

toy experiments were generated correspond<strong>in</strong>g to each of the three samples. Each experiment is fit with<br />

the likelihood function used <strong>in</strong> the branch<strong>in</strong>g ratio analysis with the usual PDFs for Ñ�Ë, ¡�, and � and<br />

the appropriate re-parameterized Fisher PDF based on the � Ó× �Ë� cut. Events are generated with Poisson<br />

statistics correspond<strong>in</strong>g to the published Run 1 result (see Sec. 7.2), scaled up to fb and modified by the<br />

relative efficiency of the different Ó× �Ë cuts. The signal efficiency is obta<strong>in</strong>ed assum<strong>in</strong>g a flat distribution,<br />

while the background efficiency is obta<strong>in</strong>ed from the on-resonance Ñ�Ë side-band data.<br />

Figure 7-2 shows the distribution of fitted �� yield divided by its error, which is an estimate of Ë� Ô Ë �,<br />

for each of the toy samples. The �� and �� samples give the same significance, while the �� sample is less<br />

optimal. The cut at �� removes � of the background and leads to more Gaussian Fisher distributions.<br />

The reduction <strong>in</strong> background means that the time-dependent fits and toy Monte Carlo studies run twice as<br />

fast, which is not an <strong>in</strong>significant advantage. We have therefore decided to use � Ó× �Ë� � �� as our default<br />

cut.<br />

ANALYSIS OF THE TIME-DEPENDENT �È -VIOLATING ASYMMETRY IN � � � � DECAYS

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