development of micro-pattern gaseous detectors – gem - LMU
development of micro-pattern gaseous detectors – gem - LMU
development of micro-pattern gaseous detectors – gem - LMU
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Introduction<br />
Our universe is momentarily described by the standard model [Grif 08]. It contains three generations<br />
<strong>of</strong> leptons consisting <strong>of</strong> electron, muon, tau and their corresponding neutrinos and six quarks, namely<br />
the up and down, charm and strange as well as top and bottom. They represent the fermions, spin 1<br />
2 -<br />
particle.<br />
Interactions are mediated via bosons: the photon responsible <strong>of</strong> the electromagnetic interaction, the<br />
W − , W + and Z bosons for the weak interaction and eight gluons as carrier <strong>of</strong> the strong force.<br />
Figure 1: The LHC near Geneva and the installed experiments [CERN 10].<br />
About 100 m deep underground in the Large Hadron Collider at CERN 1 (cf. Fig 1) near Geneva<br />
protons collide at center-<strong>of</strong>-mass energies <strong>of</strong> up to 14 TeV to further investigate nature. A main<br />
interest is the question <strong>of</strong> the generation <strong>of</strong> mass that is supposed to result from the Higgs mechanism.<br />
To study the physics <strong>of</strong> these collisions, <strong>detectors</strong> are installed around the beam interaction points.<br />
One <strong>of</strong> them is the ATLAS 2 detector, shown in Fig. 2. It is a multi purpose detector <strong>of</strong> 44 m length<br />
and 25 m height that detects the reaction products <strong>of</strong> proton collisions designed to occur every<br />
25 ns [ATLA 10]. The detector has a multi layer structure beginning with the inner tracking <strong>detectors</strong><br />
(“SCT 3 ”, “Pixel Detector” and “TRT 4 ” in Fig. 2) near the collision point and in a solenoid magnetic<br />
1 European Organization for Nuclear Research<br />
2 A Toroidal LHC AS<br />
3 Semi Conductor Tracker<br />
4 Transition Radiation Tracker<br />
1