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Measurement of the Jet Energy Scale in the CMS experiment ... - IIHE

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CHAPTER 2: The <strong>CMS</strong> <strong>experiment</strong> at <strong>the</strong> LHC 19The results <strong>of</strong> analyz<strong>in</strong>g <strong>the</strong> 36.1 pb −1 <strong>of</strong> <strong>the</strong> proton-proton collision data <strong>in</strong> <strong>the</strong>framework <strong>of</strong> this <strong>the</strong>sis are given <strong>in</strong> detail <strong>in</strong> Section 5.6.Currently <strong>the</strong> LHC mach<strong>in</strong>e is operat<strong>in</strong>g at a center <strong>of</strong> mass energy <strong>of</strong> 7 TeV and <strong>the</strong><strong>CMS</strong> <strong>experiment</strong> has already been able to record an <strong>in</strong>tegrated lum<strong>in</strong>osity <strong>of</strong> protoncollisions equivalent to more than 2000 pb −1 = 2 fb −1 <strong>in</strong> 2011, hence 55 times moredata than what had been collected <strong>in</strong> 2010. The LHC has been designed to operateat an even higher center <strong>of</strong> mass energy, be<strong>in</strong>g two times larger than <strong>the</strong> one achieved.It has been decided [36, 37] that <strong>the</strong> mach<strong>in</strong>e cont<strong>in</strong>ues runn<strong>in</strong>g at a center <strong>of</strong> massenergy <strong>of</strong> 7 TeV at least until <strong>the</strong> end <strong>of</strong> 2011.2.1.2 Particle Detectors at <strong>the</strong> LHCFour ma<strong>in</strong> <strong>experiment</strong>s detect collisions which occur at <strong>the</strong> LHC. Two <strong>of</strong> <strong>the</strong>m, be<strong>in</strong>g<strong>CMS</strong> (Compact Muon Solenoid) [38] and ATLAS (A Toroidal LHC ApparatuS) [39],are general-purpose detectors. They are designed to address a wide variety <strong>of</strong> physicsquestions. Search<strong>in</strong>g for <strong>the</strong> Higgs particle, explor<strong>in</strong>g physics at TeV scale and look<strong>in</strong>gfor evidence <strong>of</strong> physics beyond <strong>the</strong> Standard Model such as supersymmetry are some<strong>of</strong> <strong>the</strong> goals which are followed by <strong>the</strong> multi-purpose <strong>experiment</strong>s <strong>of</strong> <strong>the</strong> LHC.The o<strong>the</strong>r two, ALICE (A Large Ion Collider Experiment) [40] and LHCb (LargeHadron Collider beauty) [41], are special-purpose detectors. While <strong>the</strong> former is dedicatedto heavy ion collisions, <strong>the</strong> latter is specialized to <strong>the</strong> studies <strong>of</strong> b quark physics.The location <strong>of</strong> <strong>the</strong>se ma<strong>in</strong> <strong>experiment</strong>s around <strong>the</strong> ma<strong>in</strong> r<strong>in</strong>g <strong>of</strong> <strong>the</strong> LHC is shown <strong>in</strong>Figure 2.3.In addition to <strong>the</strong> four ma<strong>in</strong> <strong>experiment</strong>s, <strong>the</strong> LHC hosts two more detectors. Afirst one, which is named LHCf (Large Hadron Collider forward) [42], is <strong>in</strong>tended tostudy <strong>the</strong> particles that are produced <strong>in</strong> <strong>the</strong> forward region <strong>of</strong> <strong>the</strong> <strong>in</strong>teraction po<strong>in</strong>t<strong>of</strong> proton collisions. It consists <strong>of</strong> two pieces which are <strong>in</strong>stalled on ei<strong>the</strong>r side <strong>of</strong> <strong>the</strong>ATLAS detector, 140 m away from <strong>the</strong> <strong>in</strong>teraction po<strong>in</strong>t. A second one, which is namedTOTEM (TOTal Elastic and diffractive cross section <strong>Measurement</strong>) [43], is designedto measure <strong>the</strong> total proton-proton cross section. It is located on <strong>the</strong> forward region<strong>of</strong> <strong>the</strong> <strong>CMS</strong> detector.2.2 The <strong>CMS</strong> ExperimentDetectors are constructed <strong>in</strong> order to observe and analyze <strong>the</strong> collisions which are providedby <strong>the</strong> collider. Explor<strong>in</strong>g <strong>the</strong> vast physics opportunities <strong>in</strong> <strong>the</strong> proton-protoncollisions at high energy scales reachable at <strong>the</strong> LHC, requires to build general-purposeparticle detectors such as <strong>the</strong> <strong>CMS</strong> <strong>experiment</strong>. Particle detectors are generally designedto be symmetric <strong>in</strong> space to make <strong>the</strong> physics analysis easier. The particle isdetected when it <strong>in</strong>teracts with matter. Accord<strong>in</strong>g to <strong>the</strong> various k<strong>in</strong>d <strong>of</strong> particle <strong>in</strong>teractions,<strong>the</strong> detectors conta<strong>in</strong> appropriate materials, each <strong>of</strong> which is aimed to identifysome special type <strong>of</strong> particles or to measure particular properties <strong>of</strong> <strong>the</strong> particles. Thesub-systems are arranged <strong>in</strong> such a way which yields <strong>the</strong> detector to have an onion-likestructure. A slice <strong>of</strong> <strong>the</strong> transverse view <strong>of</strong> <strong>the</strong> <strong>CMS</strong> detector is shown <strong>in</strong> Figure 2.5.

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