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 2: The Accelerator and <strong>the</strong> Experiment 39<br />
two endcap <strong>section</strong>s. Toge<strong>the</strong>r, <strong>the</strong>y provide <strong>the</strong> magnetic field necessary for charged<br />
particle momentum measurement over a volume <strong>of</strong> 12,000 m 3 . A schematic <strong>of</strong> <strong>the</strong><br />
ATLAS magnet system is shown <strong>in</strong> Figure 2.3.<br />
The central solenoid provides a 2T axial magnetic field for <strong>the</strong> <strong>in</strong>ner detector.<br />
Charged particles bend <strong>in</strong> <strong>the</strong> r − φ plane. The w<strong>in</strong>d<strong>in</strong>g is made <strong>of</strong> Al-stabilised<br />
NbTi alloy, cooled to 4.5 K us<strong>in</strong>g liquid helium. The diameter and axial length <strong>of</strong><br />
<strong>the</strong> solenoid are 2.5 m and 5.3 m respectively, and stores 40 MJ <strong>of</strong> energy at <strong>the</strong><br />
full current <strong>of</strong> 7330 A. The material <strong>of</strong> <strong>the</strong> solenoid is equivalent to ≈ 0.66 radiation<br />
lengths at normal <strong>in</strong>cidence.<br />
In <strong>the</strong> toroid, <strong>the</strong> magnetic field is along <strong>the</strong> φ coord<strong>in</strong>ate, so that charged particles<br />
bend <strong>in</strong> <strong>the</strong> r − z plane. The barrel toroid has eight racetrack-shaped coils arranged<br />
symmetrically <strong>in</strong> <strong>the</strong> azimuth. It has <strong>in</strong>ner and outer diameters <strong>of</strong> 9.4 m and 20.1<br />
m respectively, and a length <strong>of</strong> 25.3 m. The endcap toroids each conta<strong>in</strong> eight flat<br />
coil units and eight keystone wedges bolted and glued toge<strong>the</strong>r. Each unit is 5 m <strong>in</strong><br />
length. At <strong>the</strong> peak current <strong>of</strong> 20.5 kA, <strong>the</strong> barrel and endcap toroids provide average<br />
fields <strong>of</strong> 0.5 T and 1 T respectively, and have a comb<strong>in</strong>ed stored energy <strong>of</strong> 1.58 GJ.<br />
In order to m<strong>in</strong>imize multiple scatter<strong>in</strong>g, <strong>the</strong> toroids were designed with a air core<br />
ra<strong>the</strong>r than us<strong>in</strong>g iron to enhance <strong>the</strong> magnetic field.<br />
Dur<strong>in</strong>g operation, each coil <strong>of</strong> <strong>the</strong> barrel toroid experiences an <strong>in</strong>ward Lorentz<br />
force <strong>of</strong> about 1400 tons [98]. This force is balanced by Al alloy struts <strong>in</strong> between<br />
<strong>the</strong> eight coils. In <strong>the</strong> case <strong>of</strong> <strong>the</strong> endcap toroids, <strong>the</strong> force is counteracted by stops<br />
mounted on <strong>the</strong> eight barrel toroid coils.