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Violation in Mixing

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198 Analysis of the time-dependent �È -violat<strong>in</strong>g asymmetry <strong>in</strong> � � � � decays<br />

�� �� ���<br />

Parameter � � � � � �<br />

�Ñ�Ë � �� � �� � �� � �� � � � �<br />

�Ñ�Ë � �� � � � �� � ��� � � � ���<br />

�¡� � �� � � � � � � ��� � ���<br />

�¡� � �� � �� � �� � ��� � � � �<br />

� offsets (Run 1) � � � � ��� � �� � � � � �<br />

� offsets (Run 2) � � � � ��� � � � ��� � ���<br />

�� (Run 1) � �� � �� � �� � � � � �� �<br />

�� (Run 2) � �� � � � � � � � � � � �<br />

Table 7-24. Systematic errors due to uncerta<strong>in</strong>ties <strong>in</strong> the signal Ñ �Ë, ¡�, and � parameterizations.<br />

�� �� ���<br />

Parameter � � � � � �<br />

Lepton � � � � � � � � � ��<br />

Kaon � � � � � �� � �� � � � ��<br />

NT1 � � � �� � �� � � � �<br />

NT2 � � � � � � � � �<br />

Table 7-25. Systematic errors due to signal tagg<strong>in</strong>g efficiencies.<br />

f<strong>in</strong>d �� � � and � à ¦ � § candidates and measure:<br />

�� � �<br />

��� � � �<br />

��<br />

���<br />

���<br />

���<br />

¦ � �<br />

¦ � ��<br />

�Ã� � � � ¦ � � ¦ � �<br />

where the first error is statistical and the second is systematic. The systematic error on �� is the quadrature<br />

sum of the total from Table 7-32 and an uncerta<strong>in</strong>ty of ¦ � from possible charge bias <strong>in</strong> track reconstruction<br />

and particle identification [6]. We calculate the � confidence limit on �Ã�, � � � � �℄, <strong>in</strong>clud<strong>in</strong>g<br />

the statistical and systematic errors and assum<strong>in</strong>g Gaussian errors.<br />

To conclude, even if this result is still statistically limited, the analysis method is demonstrated to be robust<br />

and promis<strong>in</strong>g as soon as a higher statistics is available.<br />

MARCELLA BONA

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