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Violation in Mixing

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6<br />

Measurement of Branch<strong>in</strong>g Fractions for<br />

� � Ã Ë Ã Ë Decays<br />

This chapter describes the charmless two-body analyses for all-neutral f<strong>in</strong>al state conta<strong>in</strong><strong>in</strong>g Ã Ë mesons.<br />

The latest results from CLEO [65] on decays with all-neutral f<strong>in</strong>al state is � � � Ã Ã � � ¢ � .<br />

6.1 Data samples and event selection<br />

The analyses presented <strong>in</strong> this chapter use the data samples described <strong>in</strong> Sec. 4.1 and the selection described<br />

<strong>in</strong> Sec. 4.2. Issues related to reconstruction of Ã Ë mesons have been discussed <strong>in</strong> Sec. 5.2. For the Ã Ë we<br />

require ØÃË��Ø � �, where ØÃË is the measured (2-d) decay time and �Ø is its error. The mass w<strong>in</strong>dow is<br />

¬ � � Å�Î� ( ���).<br />

tightened to ¬ ¬ Å � � Å Ã Ë<br />

� mesons are constructed by comb<strong>in</strong><strong>in</strong>g two ÃË candidates. To choose between multiple candidates <strong>in</strong> the<br />

same events, we use the variable Æ � ¡Å<br />

ÃË<br />

value of Æ.<br />

¡Å<br />

ÃË<br />

� and we keep the candidates with the smallest<br />

We use the k<strong>in</strong>ematic variables Ñ�Ë and ¡�. We require �� � Ñ�Ë � �� ��Î� and �¡�� �<br />

� ��Î. From the conservative ¡� resolution value of � Å�Î, the signal region is def<strong>in</strong>ed as �¡�� �<br />

� ��Î (i.e. 4 times the ¡� resolution). The regions � � ¡� � � ��Î and � � ¡� �<br />

� ��Πare referred to as the lower and upper side-bands, respectively, and each of them has the same<br />

width of the signal region (0.2 ��Î).<br />

We also create a control sample collect<strong>in</strong>g those events rejected by the � Ó× �Ë� cut, <strong>in</strong> order to study the<br />

ARGUS function shape <strong>in</strong> different ranges of �¡�� values.<br />

6.2 Analysis strategy<br />

Previous experiments have found no evidence of the decay � � ÃËÃË: the theoretical expectation for<br />

the � � Ã Ã branch<strong>in</strong>g ratio is less than � , but consider<strong>in</strong>g the efficiency, given that we reconstruct<br />

à � Ã Ë � � � , we expect to see Ã Ë Ã Ë events with an effective branch<strong>in</strong>g ratio less than � . S<strong>in</strong>ce<br />

we aim for sett<strong>in</strong>g the lowest upper limit possible on the branch<strong>in</strong>g ratio measurement, we have <strong>in</strong>vestigated<br />

two possible strategies to search for this channel <strong>in</strong> the BABAR data sample: the usual global likelihood<br />

technique and a count<strong>in</strong>g analysis optimization. With a toy Monte Carlo <strong>in</strong> the first case and with the on-

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