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Violation in Mixing

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50 The BABAR Experiment<br />

design value achieved value<br />

HER energy �� ��Î �� ��Î<br />

LER energy � ��Î � ��Î<br />

# of bunches ��� �� � �<br />

bunch spac<strong>in</strong>g �� Ò× �� �� Ò×<br />

positron current � mA � mA<br />

electron current �� mA � � mA<br />

�Ü �Ñ �Ñ<br />

�Ý � �Ñ ��� �Ñ<br />

lum<strong>in</strong>osity � cm s �� cm s<br />

<strong>in</strong>tegrated day lum<strong>in</strong>osity � pb �� �� pb ��<br />

Table 2-1. Design and achieved mach<strong>in</strong>e parameters.<br />

The beam energies of the two beams are calculated from the total magnetic bend<strong>in</strong>g strength and the average<br />

deviations of the accelerat<strong>in</strong>g frequencies from their central values. The systematic error on the PEP-II<br />

calculation of the absolute beam energies is estimated to be � Å�Î, while the relative energy sett<strong>in</strong>g<br />

for each beam is accurate and stable to about Å�Î.<br />

Cross sections for the production of fermion pairs at the § �Ë mass energy (which is Ô × � Å § �Ë �<br />

��� ��Î) are shown <strong>in</strong> table 2-2.<br />

� � � cross sections (nb)<br />

�� (� �� ) � �<br />

(� ) �<br />

×× (�××) � �<br />

ÙÙ (�ÙÙ) � �<br />

�� (� �� ) � �<br />

� � (�� ) ���<br />

� � (��) � �<br />

� � (��) � �<br />

Table 2-2. Cross sections � for the production of fermion pairs at the § �Ë mass energy.<br />

BABAR has accumulated ��� fb <strong>in</strong> year 2000 and �� fb <strong>in</strong> 2001 until November: Fig. 2-2 shows the<br />

<strong>in</strong>tegrated lum<strong>in</strong>osity <strong>in</strong>clud<strong>in</strong>g 1999, 2000 and 2001 periods and the BABAR efficiency <strong>in</strong> the same periods.<br />

MARCELLA BONA

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