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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 />

6<br />

122 Analysis of Run 10<br />

rate (event / 8 hr file)<br />

0.4<br />

0.35<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

15/07<br />

2008<br />

84.3 d<br />

all data<br />

without the overflow<br />

29/07<br />

2008<br />

12/08<br />

2008<br />

26/08<br />

2008<br />

09/09<br />

2008<br />

23/09<br />

2008<br />

all data<br />

07/10<br />

2008<br />

21/10<br />

2008<br />

rate (event / 8 hr file)<br />

Figure 6.2: Rate of the muon veto per 8-hour file when the veto is closed, see text<br />

for <strong>de</strong>tails. The rate is shown over time (left) and as a histogram (right) with a<br />

Gaussian fit. The points with a much smaller rate are from fi<strong>les</strong> <strong>les</strong>s than 8-hours<br />

long. In lighter sha<strong>de</strong> is the rate without the very high energy events. The mean of<br />

the Gaussian fit is 0.161 Hz (calculated rate from data is also 0.161 Hz).<br />

t t10µs (10 µs)<br />

10µs (10 µs)<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

x10 9<br />

0 200<br />

400 600 800 1000 1200<br />

event number<br />

events per 25 ms<br />

x10 3<br />

per 0.8 ms<br />

04/11<br />

2008<br />

18/11<br />

2008<br />

(s)<br />

∆t veto (s)<br />

Figure 6.3: Left: Timeline of the veto events during Run 10, with the condition<br />

of having a time difference of consecutive events lower than 600 s. The timeline is<br />

broken twice when the muon veto DAQ was stopped, due to the installation of the<br />

neutron counter, see also Figure 6.2. Right: Time difference of consecutive muon<br />

veto events in log scale up to 10 s and zoomed over the first four 25 ms. At −0.25 s<br />

are plotted ∆tveto > 600 s, at −0.75 s are plotted ∆tveto < 0 s.

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