Violation in Mixing
Violation in Mixing
Violation in Mixing
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7<br />
Analysis of the time-dependent<br />
�È -violat<strong>in</strong>g asymmetry <strong>in</strong><br />
� � � � decays<br />
This chapter describes the analysis of the time evolution <strong>in</strong> � � � � decays. In the Standard Model, the<br />
time-dependent �È -violat<strong>in</strong>g asymmetry <strong>in</strong> � � � � is related to the angle « of the Unitarity Triangle<br />
(Sec. 1.5.3.1). This decay mode has only recently been observed by CLEO [67] and confirmed by BaBar [6]<br />
and Belle [68]. Due to the small decay rate (�Ê � � ¢ � ), large cont<strong>in</strong>uum ÕÕ background, and significant<br />
cross-feed from � � à � decays, extraction of the �È asymmetry <strong>in</strong> � � is <strong>in</strong>timately related<br />
to the branch<strong>in</strong>g fraction measurement. In addition, this measurement relies heavily on the <strong>in</strong>frastructure<br />
(tagg<strong>in</strong>g [69] and vertex<strong>in</strong>g [71] <strong>in</strong> particular) developed for the ×�Ò ¬ analysis [72].<br />
7.1 �È analysis requirements<br />
The formalism has been already described <strong>in</strong> the Sec. 1.5. Def<strong>in</strong><strong>in</strong>g ¡Ø � Ø�È ØØ��, where Ø�È and ØØ��<br />
are the proper decay times of the �È and tagged �’s, respectively, the decay rate distribution � � (<strong>in</strong><br />
Eq. 1.34) for ��È � � when �Ø�� is a � � can be rewritten as:<br />
�¡Ø��� �<br />
�¦ ¡Ø �<br />
��<br />
where � is the average � lifetime, ¡Ñ�� is the mix<strong>in</strong>g frequency, and<br />
� ¦ Ë� ×�Ò ¡Ñ�� ¡Ø § �� Ó× ¡Ñ�� ¡Ø ℄ � (7.1)<br />
Ë� � ÁÑ�<br />
��� �� �� � ���<br />
���<br />
� (7.2)<br />
Interference effects are <strong>in</strong>cluded <strong>in</strong> the physical quantity �, def<strong>in</strong>ed <strong>in</strong> Eq. 1.22 or <strong>in</strong> 1.41: it can be rewritten<br />
as<br />
� � Õ ��<br />
� �� �<br />
Ô ��<br />
�� �� � (7.3)<br />
��<br />
where � �� is the weak mix<strong>in</strong>g phase, �� �� is the amplitude for the decay � � � � � � , �� is the<br />
�È eigenvalue of the f<strong>in</strong>al state, and the assumption of no �È violation <strong>in</strong> mix<strong>in</strong>g (�Õ�Ô� � ) is implicit. In<br />
this ¬ analysis, observable �È violation effects can arise from <strong>in</strong>terference between different decay amplitudes<br />
¬<br />
¬ ( ¬� ��� � ¬ �� ) and <strong>in</strong>terference between the mix<strong>in</strong>g and decay weak phases (see Sec. 1.3.3).