Measurement of the Z boson cross-section in - Harvard University ...
Measurement of the Z boson cross-section in - Harvard University ...
Measurement of the Z boson cross-section in - Harvard University ...
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Chapter 3: Lum<strong>in</strong>osity <strong>Measurement</strong> at <strong>the</strong> LHC and <strong>in</strong> ATLAS 80<br />
The synchrotron light source can also be used to measure bunch length and <strong>the</strong><br />
longitud<strong>in</strong>al beam pr<strong>of</strong>ile. Part <strong>of</strong> <strong>the</strong> synchrotron radiation generated by <strong>the</strong> undu-<br />
lators is collected by a separate mirror located beh<strong>in</strong>d <strong>the</strong> transverse optics. About<br />
2 × 10 6 photons are expected to be collected for each bunch <strong>of</strong> 1.15 × 10 11 protons.<br />
The photon flux reproduces <strong>the</strong> time and <strong>in</strong>tensity pr<strong>of</strong>iles <strong>of</strong> <strong>the</strong> beam, so that lon-<br />
gitud<strong>in</strong>al measurements can be made.<br />
3.2.4 Beam position monitors<br />
Beam position monitors (BPMs) measure <strong>the</strong> transverse position <strong>of</strong> <strong>the</strong> beam,<br />
and are used extensively <strong>in</strong> any accelerator complex. Inside l<strong>in</strong>acs and transfer l<strong>in</strong>es,<br />
<strong>the</strong>y are used to measure and correct beam trajectories. They also measure beam<br />
trajectories <strong>in</strong>side synchrotrons. In particular, <strong>the</strong> first turn trajectory measurement<br />
is vital for clos<strong>in</strong>g <strong>the</strong> orbit on itself. Once a closed orbit has been established, BPMs<br />
cont<strong>in</strong>uously monitor beam position on a turn-by-turn or even bunch-by-bunch basis.<br />
Data from <strong>the</strong> BPMs is used for beam-related measurements such as Van der Meer<br />
scans.<br />
The basic concept beh<strong>in</strong>d most BPMs is electrostatic or electromagnetic pickup<br />
from <strong>the</strong> beam by devices placed <strong>in</strong>side <strong>the</strong> beam-pipe. We will briefly describe <strong>the</strong><br />
most commonly used beam pick-up technology at <strong>the</strong> LHC, namely button pickups.<br />
Button pickups: These are electrostatic pickups with button-shaped electrodes,<br />
thus <strong>the</strong> name (Figure 3.8). As a beam <strong>of</strong> charged particles travels along <strong>the</strong> metal<br />
beampipe, it <strong>in</strong>duces an image charge on <strong>the</strong> pipe wall. The image charge mimics <strong>the</strong><br />
longitud<strong>in</strong>al pr<strong>of</strong>ile <strong>of</strong> <strong>the</strong> beam and travels at <strong>the</strong> same speed as <strong>the</strong> beam. A button