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

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

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θN [per 5°]908070hthetaEntries 649Mean 0.6072RMS 0.2375ϕN [per 20°]7060hphiEntries 649Mean 3.206RMS 2.022605050404030203020101000 0.2 0.4 0.6 0.8 1 1.2 1.4θ00 1 2 3 4 5 6ϕFigure 5.9: Zenith <strong>and</strong> azimuth angular distributions for events observed by theCMT. The filled area shows the actual data wheres the red crosses show the resultsfrom the Monte Carlo simulation.5.2 Commissioning <strong>and</strong> Early ResultsAlthough the detector was installed already in November 2009, the commissioningdid not start until late January 2010 due to a missing gas supply. Because <strong>of</strong> thelow flux <strong>of</strong> cosmic muons a check <strong>of</strong> the detector functionality takes a few daysto gather enough statistics. The detector is running at all times, however due tooccasional power cuts in the laboratory, there are some discontinuities in the data.After a power cut, data taking has to be resumed manually. In the first weeks <strong>of</strong>data taking, some <strong>of</strong> these restarts <strong>of</strong> the detector unfortunately remained unnoticedfor a couple <strong>of</strong> days. Meanwhile, an automatic email alert system has been set upsending out warning messages whenever there is a restart <strong>of</strong> the system. However,it is foreseen to connect the CMT to a UPS 1 in the near future to both ensurecontinuous data taking <strong>and</strong> to prevent the system from any damage.Data taking started on January 28 th 2010. The results presented here rely on thedata taken until the 6 th <strong>of</strong> September 2010. An overview <strong>of</strong> the runs taken duringthis period is given in Tab. 5.3. A 2D projection <strong>of</strong> a typical event is depicted inFig. 5.10 <strong>and</strong> Fig. 5.11 shows a different event in the 3D display.5.2.1 A First Look at EventsDue to the small muon rate, the overall number <strong>of</strong> events is too little for selfcalibration.Therefore, a calibration was done in Hamburg before setting up thedetector underground. Of course, this calibration suffers from the different ambientconditions in the laboratories in Hamburg <strong>and</strong> Gran Sasso, the main differencesbeing pressure <strong>and</strong> temperature. Three attempts <strong>of</strong> a calibration have been made:First, a reconstruction was done with the original CMT calibration from the testmeasurements before shipping the detector to Gran Sasso. Second, a calibrationobtained by a similar detector setup in Hamburg which uses a gas system to control1 UPS: Uninterruptable Power Supply77

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