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Violation in Mixing

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4<br />

Strategy and Tools for Charmless Two-body<br />

� Decays Analysis<br />

This chapter describes the requirements, the techniques and the variables common to all the hadronic<br />

charmless two-body analyses. These analyses refer to those � decays that do not <strong>in</strong>clude quarks <strong>in</strong> the<br />

f<strong>in</strong>al states and whose f<strong>in</strong>al states are made up of two particles among charged and neutral � and charged<br />

and neutral Ã.<br />

Crucial issues <strong>in</strong> the hadronic charmless two-body modes are background fight<strong>in</strong>g and particle identification<br />

(where applicable). The ma<strong>in</strong> background to these decays is due to fake � candidates reconstructed <strong>in</strong> the<br />

cont<strong>in</strong>uum � � � ÕÕ production (see Tab. 2-2). This background contam<strong>in</strong>ation together with the small<br />

expected branch<strong>in</strong>g fractions and the relatively large ÕÕ cross section, would not allow for high purity values<br />

while keep<strong>in</strong>g reasonable efficiencies.<br />

In order to reach a good discrim<strong>in</strong>at<strong>in</strong>g power aga<strong>in</strong>st background, CLEO approach has been adopted [46]: a<br />

Fisher discrim<strong>in</strong>ant [47] has been developed and studied to separate signal from background on a statistical<br />

basis. S<strong>in</strong>ce the charged tracks result<strong>in</strong>g from charmless two-body � decays have relatively high momenta<br />

(approximately �� �� ��Î� ), the � ��Ö�Ò�ÓÚ angle � , determ<strong>in</strong>ed from the �ÁÊ�(Sec.‘2.2.4), is the<br />

only measurement which provides good à � discrim<strong>in</strong>ation.<br />

A maximum likelihood fit is used to measure the yields <strong>in</strong> the various channels from the data sample. The fit<br />

<strong>in</strong>corporates the Fisher output and k<strong>in</strong>ematic variables of the � candidate, which are used to separate signal<br />

and background, as well as the � ��Ö�Ò�ÓÚ angle (where applicable), which is used to dist<strong>in</strong>guish between<br />

the channels conta<strong>in</strong><strong>in</strong>g a � or a Ã.<br />

A second method, a count<strong>in</strong>g analysis, is used as a cross check <strong>in</strong> the measurement of the decay rates (see<br />

Sec. 4.6).<br />

4.1 Data samples<br />

The full so called Run 1 data-set is used <strong>in</strong> the analyses described <strong>in</strong> the follow<strong>in</strong>g chapters. The detailed<br />

data sample used is:<br />

¯ �� ¦ � fb of on-resonance data correspond<strong>in</strong>g to �� ¦ �� ¢ � �� events.<br />

¯ �� ¦ � � fb off-resonance

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