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Violation in Mixing

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52 The BABAR Experiment<br />

3-95<br />

7857A21<br />

Q4<br />

0.653<br />

Q2<br />

1120<br />

150<br />

100<br />

Q1<br />

1655<br />

460<br />

1113<br />

330<br />

6290<br />

3750<br />

800<br />

Coil Cryostat 100<br />

Calorimeter<br />

1657<br />

Q1<br />

2395<br />

Figure 2-3. The BABAR detector.<br />

10<br />

500<br />

36<br />

150<br />

1120<br />

1730<br />

1400<br />

1360<br />

36<br />

.249 ref.<br />

900<br />

890<br />

810<br />

225<br />

Q2<br />

The �È decay modes of <strong>in</strong>terest generally have �Ê below � and reconstruct<strong>in</strong>g them requires observ<strong>in</strong>g<br />

anywhere two to six charged particles: <strong>in</strong> order to get a good efficiency, the BABAR detector has to cover as<br />

much solid angle as possible. As PEP-II is an asymmetric collider, particular care must be taken to cover<br />

the forward region: the applied boost implies that, on average, half the produced particles are <strong>in</strong> the region<br />

with Ó× �Ð�� � ��. The accelerator bend<strong>in</strong>g magnets limit the maximum acceptance to �� Æ , <strong>in</strong> both<br />

forward and backward directions, but to allow the maximum forward coverage, mach<strong>in</strong>e components such<br />

as cool<strong>in</strong>g systems etc, are located <strong>in</strong> the backward region. The active parts of the silicon vertex tracker cover<br />

the polar angle between � Æ and � � Æ <strong>in</strong> the laboratory frame. This region <strong>in</strong> the lab frame corresponds<br />

to ��� � Ó× ��Å � ��� where ��Å is the polar angle <strong>in</strong> the center-of-mass frame.<br />

Another important parameter is the m<strong>in</strong>imum measurable momentum value for both charged and neutral particles:<br />

tak<strong>in</strong>g <strong>in</strong>to consideration that charged pions have m<strong>in</strong>imum momentum values of about ��<br />

and that tagg<strong>in</strong>g kaons have m<strong>in</strong>imum momentum values of about � ���, the track<strong>in</strong>g system has a<br />

m<strong>in</strong>imum acceptance value of � �� for momenta. In case of photons, the energy spectra have shown<br />

that the m<strong>in</strong>imum measurable energy value must be � Å�Î.<br />

MARCELLA BONA

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