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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 38<br />

η = −ln[tan θ].<br />

The ATLAS detector was designed to have uniform segmentation <strong>in</strong><br />

2<br />

η and φ to exploit <strong>the</strong>se properties <strong>of</strong> hadronic collisions.<br />

Figure 2.2: A cutaway view <strong>of</strong> <strong>the</strong> ATLAS detector. The dimensions and <strong>the</strong> different<br />

subsystems are <strong>in</strong>dicated.<br />

Reference [98] presents an extensive overview <strong>of</strong> all aspects <strong>of</strong> <strong>the</strong> detector. The<br />

follow<strong>in</strong>g <strong>section</strong>s summarize <strong>the</strong> salient features <strong>of</strong> each subsystem and <strong>of</strong> <strong>the</strong> trigger<br />

and data acquisition systems.<br />

2.2.1 The magnet system<br />

The overall design <strong>of</strong> ATLAS was largely determ<strong>in</strong>ed by <strong>the</strong> choice <strong>of</strong> <strong>the</strong> magnet<br />

system, which consists <strong>of</strong> a superconduct<strong>in</strong>g solenoid surround<strong>in</strong>g <strong>the</strong> <strong>in</strong>ner detector<br />

and a superconduct<strong>in</strong>g air-core toroid for <strong>the</strong> muon system that has a barrel and

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