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Etude de bruit de fond induit par les muons dans l'expérience ...

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tel-00724955, version 1 - 23 Aug 2012<br />

4.5 Tracking muon candidates 89<br />

si<strong>de</strong> orientation 〈Esimu〉 (MeV) ELMPV (ADC-ch)<br />

upper level Top horizontal 11.8 686.8<br />

North vertical (ss) 20.8 (1.8) 1254.3 (1.8)<br />

South vertical (ss) 20.7 (1.7) 1269.0 (1.8)<br />

NEMO vertical (ls) 23.7 (2.9) 1565.5 (2.3)<br />

East vertical (ls) 24.0 (2.0) 1887.3 (2.7)<br />

lower level East vertical (ls) 23.8 (2.0) 1984.7 (2.8)<br />

South vertical (ls) 19.6 (1.7) 1914.0 (2.8)<br />

North vertical (ls) 19.9 (1.7) 1719.8 (2.5)<br />

NEMO vertical (ls) 23.9 (2.0) 1670.7 (2.4)<br />

Bottom horizontal 12.2 (1.0) 1263.2 (1.8)<br />

Table 4.2: Mean muon energy <strong>de</strong>posit (simulation and experimental) in plastic<br />

scintillator modu<strong>les</strong> for different orientation in the EDELWEISS-II setup. Vertical<br />

modu<strong>les</strong> are laid out either on the short si<strong>de</strong> (ss) or on the long si<strong>de</strong> (ls). In brackets<br />

are the relative contribution of a si<strong>de</strong> com<strong>par</strong>e to the Top one. The muon generation<br />

is from [184]. The measured LPMV is for muon candidates of a si<strong>de</strong> of a level, which<br />

are in coinci<strong>de</strong>nce with the other level. This com<strong>par</strong>ison works only if all modu<strong>les</strong><br />

are perfectly calibrated to the same gain, which is not the case.<br />

on their length (4 m , 3.75 m, 3.15 m and 2 m) rather than individually to increase<br />

the statistics. The resulting spectrum of the time difference coming from both ends<br />

of a module is shown per set in Figure 4.5. Each end of a spectrum can be fit by<br />

a Gaussian function. The size of the module is set to correspond to the number of<br />

channels between the two Gaussian fits at mid-height:<br />

4 m module ≡ 76 TDC-ch (4.6)<br />

3.75 m module ≡ 68 TDC-ch (4.7)<br />

3.15 m module ≡ 60 TDC-ch (4.8)<br />

2 m module ≡ 36 TDC-ch (4.9)<br />

The spatial resolution of a module is <strong>de</strong>fined looking at the time difference of<br />

coinci<strong>de</strong>nces between a module n and its neighbor n + 1 of one level and further<br />

in coinci<strong>de</strong>nce with the other level of the veto system. Three sets of modu<strong>les</strong> are<br />

now <strong>de</strong>fined <strong>de</strong>pending on their position: Top modu<strong>les</strong>, vertical modu<strong>les</strong> along their<br />

shorter si<strong>de</strong> (North and South of the upper level), and vertical modu<strong>les</strong> along their<br />

longer si<strong>de</strong> (North and South of the lower level, and East and NEMO). The biplot<br />

of the time difference within the neighboring module n+1 versus the time difference<br />

within module n is shown per set in Figure 4.6. The width of this biplot distribution<br />

is the spatial resolution of a type of modu<strong>les</strong>. The projection of the biplot can be fit<br />

by a Gaussian with a width of 2σ. The resolutions obtained are in TDC channels:<br />

σtop = 10.20 TDC-ch (4.10)<br />

σss = 10.33 TDC-ch (4.11)<br />

σls = 6.53 TDC-ch (4.12)<br />

The sets <strong>de</strong>fined per size are associated to the sets <strong>de</strong>fined per position. The 4 m<br />

module are modu<strong>les</strong> from the Top si<strong>de</strong> and the North and South lower si<strong>de</strong>s, they<br />

have a resolution σtop. The 3.15 m modu<strong>les</strong> are the vertical modu<strong>les</strong> along their<br />

4

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