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Setup of a Drift Tube Muon Tracker and Calibration of Muon ...

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yyxxα0: 3.439729, α1: 6.001542, θ: 0.399388, ϕ: 5.527881nhit0: 8/8, nhit1: 8/8Event: 52, Entry: 50, Time: Sun Oct 24 11:01:58 2083Figure 3.13: Left: quasi online display <strong>of</strong> a muon event (Event 52 from RUN 063 18-33-59). A hit tube is filled with a color indicating the signal width, yellow meaningwidth=3. The solid circles correspond to the drift times. Right: the same event afterreconstruction. Different colors indicate the different 2D-planes. The event time inthe display is not correct since the data was taken before the modification <strong>of</strong> the clockemulation data to UNIX time (cf. Section 3.3).3.8.1 Monte Carlo StudiesAt sea level, the angular distribution <strong>of</strong> muons is proportional to cos 2 θ, where θ is thepolar angle [33]. However, the muon tracker only has a limited angular acceptance.To be able to compare measurements to the expectations a Monte Carlo study hasbeen performed. <strong>Muon</strong>s are generated at a fixed height z = 220 mm. This is wherethe top scintillators are located. For each event four values are r<strong>and</strong>omly generated:x linear between -500 mm <strong>and</strong> 500 mmy linear between -500 mm <strong>and</strong> 500 mmϕ linear between 0 <strong>and</strong> 2πθ according to a cos 2 distribution between 0 <strong>and</strong> π 2 .The generation <strong>of</strong> θ is not straightforward since the r<strong>and</strong>om number generator onlyreturns homogeneously distributed values between 0 <strong>and</strong> 1. Therefore, θ has to bederived from this distribution. One also has to take into account that due to thesolid angle each value θ has to be weighted by sinθ. A r<strong>and</strong>om number r has to45

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