Violation in Mixing
Violation in Mixing
Violation in Mixing
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1.5 Determ<strong>in</strong>ation of « 43<br />
b<br />
q<br />
(a)<br />
Z<br />
q<br />
q<br />
q<br />
q<br />
(b)<br />
b q<br />
q<br />
Z<br />
C<br />
P P<br />
EW<br />
EW<br />
Figure 1-9. (a) Color-allowed �-pengu<strong>in</strong>, (b) Color-suppressed �-pengu<strong>in</strong>.<br />
Us<strong>in</strong>g the above notations, the �È asymmetry <strong>in</strong> � � � � can be expressed as<br />
ÁÑ� � � �ÁÑ<br />
�<br />
q<br />
� �« � �<br />
�<br />
�<br />
q<br />
q<br />
� (1.72)<br />
The ratio � � �� is therefore the measure of the pengu<strong>in</strong> pollution on the relationship between the angle<br />
« and the measured asymmetry. The two-triangle construction gives the magnitude and phase, ���, of this<br />
quantity, so that « can <strong>in</strong> pr<strong>in</strong>ciple be extracted cleanly, even <strong>in</strong> the presence of pengu<strong>in</strong>s.<br />
One of the ma<strong>in</strong> issues <strong>in</strong> this analysis is the rate for � � � � . Some theoretical predictions of this<br />
branch<strong>in</strong>g ratio are below or at the level of Ç � : a branch<strong>in</strong>g ratio at this order of magnitude would<br />
make its measurement very challeng<strong>in</strong>g [33, 34, 31]. These estimates assume that color suppression is<br />
significant <strong>in</strong> � decays to light mesons and small pengu<strong>in</strong>s, but if large rescatter<strong>in</strong>g effects are also present<br />
<strong>in</strong> � � ��, the branch<strong>in</strong>g ratio of � � � � may be considerably larger than expectations and the isosp<strong>in</strong><br />
analysis could then yield accurate results.<br />
Theoretically, a problem that can arise <strong>in</strong> the isosp<strong>in</strong> method is the presence of electroweak pengu<strong>in</strong>s<br />
(EWP’s) [26]: the ma<strong>in</strong> EWP contributions to � � �� come from diagrams with virtual � exchange<br />
(see Fig. 1-9). The coupl<strong>in</strong>gs of the � conta<strong>in</strong> both Á � and Á � terms and thus these diagrams<br />
contribute also to ¡Á � so that their effects pollute the tree contributions. Though, the effects of these<br />
electroweak pengu<strong>in</strong>s are expected to be small <strong>in</strong> this channel. Both the Ï and the � are color s<strong>in</strong>glet<br />
particles and thus two contributions, a color-allowed and a color-suppressed one, have to be considered for<br />
each tree or electroweak-pengu<strong>in</strong> diagram. If one <strong>in</strong>cludes both color-allowed and color-suppressed EWP’s,<br />
the � � �� amplitudes become [27]:<br />
� � � � � � Ô Ì � È�Ï È � �Ï<br />
� � � � � � Ì È � È � �Ï<br />
� � � � � � Ô � È � È�Ï È � �Ï<br />
(1.73)<br />
where Ì is the color-allowed tree contribution, � the color-suppressed tree contribution, È the gluonic<br />
pengu<strong>in</strong>, � the color-suppressed tree contribution, È�Ï the color-allowed EWP contribution and È � �Ï the<br />
color-suppressed EWP contribution. The relative orders of magnitude of all these contributions are expected<br />
to be:<br />
�È VIOLATION IN THE �� SYSTEM