Violation in Mixing
Violation in Mixing
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