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Measurement of the Z boson cross-section in - Harvard University ...

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Chapter 2: The Accelerator and <strong>the</strong> Experiment 54<br />

traverses at least three chambers, referred to as a projective tower (Figure 2.11). The<br />

total number <strong>of</strong> channels <strong>in</strong> <strong>the</strong> drift chambers is 339,000.<br />

Figure 2.9: The structure <strong>of</strong> a barrel MDT chamber. Two multilayers <strong>of</strong> drift tubes<br />

and <strong>the</strong> spacer bars can be seen. The paths <strong>of</strong> <strong>the</strong> alignment rays are shown <strong>in</strong> red.<br />

Cathode Strip Chambers (CSCs): In <strong>the</strong> very forward region, MDTs suffer<br />

from high occupancy because <strong>of</strong> <strong>the</strong> large particle flux 5 . In <strong>the</strong> pseudorapidity range<br />

2.0 < |η| < 2.7, CSCs are used <strong>in</strong>stead <strong>of</strong> MDTs on <strong>the</strong> endcap wheel closest to<br />

<strong>the</strong> <strong>in</strong>teraction po<strong>in</strong>t. The CSCs are multiwire proportional chambers. The mode <strong>of</strong><br />

operation is similar to that <strong>of</strong> drift tubes <strong>in</strong> that charged particles create avalanches<br />

<strong>of</strong> electron-ion pairs <strong>in</strong> <strong>the</strong> gas. Each chamber conta<strong>in</strong>s four alternat<strong>in</strong>g planes <strong>of</strong><br />

anode wires and cathode strips. The signal from a given track is collected on several<br />

5 The safe limit <strong>of</strong> operation for an MDT is a flux <strong>of</strong> ≈ 150 Hz/cm 2 .

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