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Violation in Mixing

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1.4 �È <strong>Violation</strong> <strong>in</strong> the Standard Model 33<br />

7–92<br />

(a)<br />

(b)<br />

Figure 1-5. The three unitarity triangles: a) Î ��Î £<br />

�×<br />

common scale.<br />

(c)<br />

� ,b)Î�×Î £<br />

��<br />

7204A4<br />

� , and c) Î��Î £<br />

��<br />

� , drawn to a<br />

�Ö�� � �Þ ��Þ � ×�Ò �Ò�Ð� ��ØÛ��Ò Ø�� ÓÒ×���Ö�� ×���× � ÁÑÞ Þ £ � Â�È�<br />

The area of the unitary triangles is constant: as a matter of fact from Eq. 1.47 one can get that Â�È is always<br />

or, us<strong>in</strong>g the Wolfenste<strong>in</strong>’s parameterization <strong>in</strong> 1.49,<br />

Â�È � × × × ×�Ò Æ (1.51)<br />

Â�È<br />

� �� � �<br />

In the Wolfenste<strong>in</strong>’s parameterization, measurements of �Î �� and �ÎÙ�� provide the constra<strong>in</strong>ts<br />

� �<br />

Î �<br />

� �<br />

Î Ù×<br />

¬<br />

¬<br />

¬ Î £ ¬ Ù� ¬<br />

Î ¬<br />

�Π�<br />

�<br />

Õ<br />

� � �<br />

Thus, measurements of �Î �� essentially determ<strong>in</strong>e �, while the constra<strong>in</strong>t from �ÎÙ�� def<strong>in</strong>es a circle <strong>in</strong> the<br />

�� � plane and when errors are taken <strong>in</strong>to account this constra<strong>in</strong>t becomes an annulus. Consider<strong>in</strong>g � �<br />

mix<strong>in</strong>g, s<strong>in</strong>ce the mix<strong>in</strong>g rates are dom<strong>in</strong>ated by virtual ØØ <strong>in</strong>termediate states (as seen <strong>in</strong> Sec. 1.2.2), � �<br />

measurements constra<strong>in</strong><br />

¡Ñ� �ÎØ�� � � � � � � � ℄�<br />

�È VIOLATION IN THE �� SYSTEM

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