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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 />

C<br />

152 Definition of the bolometer timing<br />

and<br />

C.3 An example for Run 8<br />

t 0 H + ∆tH · 0.5 + T C<br />

= t max<br />

H − ∆tH · fH + ∆tH · 0.5 + t p<br />

H − tmax H<br />

= t p<br />

H<br />

(C.4)<br />

The event chosen as example for Run 8 is the 3 rd event of the run of Jan 2 th 2008,<br />

which correspond to runntp = ia02a005, and runANA = 120205.<br />

From the data analysis file, we have the time difference of the beginning of the<br />

run and of the beginning of the ionization interval, which is for Run 8 the time of<br />

the beginning of the ionization interval:<br />

T H = t 0 I = 15019.483 ms (C.5)<br />

T H is already corrected by the factor 1.008. We also have the time of the beginning<br />

of the ionization pulse relative to the center of the ionization interval:<br />

T I = 0.68573 · 1.008 ms (C.6)<br />

From the data acquisition, i.e. the ntp file, which contain the same information<br />

than the corresponding raw data fi<strong>les</strong>, we have the time of the maximum of the<br />

filtered heat pulse:<br />

t max<br />

H<br />

Thus, it is clear that T H and t max<br />

H<br />

= 1493100 unit of the 10 µs clock<br />

= 14931.000 · 1.008 ms<br />

= 15050.448 ms (C.7)<br />

are different and have a different signification,<br />

<strong>de</strong>spite a misleading name in the bolometer analysis ANA. T H is the beginning of<br />

the ionization interval and tmax H is the maximum of the heat pulse.<br />

The time of the maximum of the heat pulse in ANA can be evaluated if we add<br />

the pre-trigger fI = 0.75 of the sample window to the time of the beginning of the<br />

ionization window:<br />

max<br />

tH ANA = t0I + ∆tI · fI · 1.008 (C.8)<br />

= T H + ∆tI · fI · 1.008<br />

= 15019.483 ms + 40.96 · 0.75 · 1.008 ms<br />

Com<strong>par</strong>ing Equations C.7 and C.9, we have tmax <br />

H<br />

= 15050.449 ms (C.9)<br />

ANA<br />

= tmax H , we find back the ntp<br />

time stamp from the time of the analysis. We are now certain that the time used in<br />

the analysis and the time used in the ntp is the same and is the one coming from the<br />

<strong>de</strong>vice which dispatch the clock in 10 µs-beat, and not some arrangements from tPC. ∗<br />

∗ About tPC, the real time read in the ntp file is tPC = 1199263394.124085, then tPC − t0 PC =<br />

1199263394.124085 − 1199263379.193085 = 14931.000 ms. Therefore tPC − t0 PC = tmax H · 10−5 still<br />

holds as it is <strong>de</strong>fined in Table C.1.

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