As a result of the differing Cherenkov ring radii from different
radiators and experimental configurations, the number of HPDs
which are used to determine the photon yield for each type varies.
The layouts are specified in Table 2.
Table 2:Summary of the different detector, optical and radiator
configurations used to study the photon yield.
Layout
Radiator
Filter
Config.
No. of
HPDs
1
Air
None
1
1
2
C4F10
None
1
1
3
C4F10
None
2
4
4
C4F10
Mylar
2
2
5
Aerogel 1
None
1
4
6
Aerogel 1
Glass
1
4
7
Aerogel 1
Mylar
1
6
8
Aerogel 2
Glass
1
4
The results from Analysis 1 for each of the above layouts are
shown in Table 3 where they are also compared
with results from simulation under the same conditions.
Table 3:The observed, background & efficiency corrected, and expected number of
detected photoelectrons for the various radiator and filter
configurations determined using Analysis 1.
Layout
Raw
Backgnd.
Efficncy.
Corr.
Corr.
1
4.92
4.56
4.80
0.90
2
7.85
7.49
34.80
1.02
3
12.83
12.77
89.46
1.05
4
1.78
1.76
24.66
1.46
5
1.79
1.31
11.39
0.73
6
1.14
0.75
6.52
0.92
7
1.34
0.81
3.71
0.64
8
0.85
0.52
4.52
1.10
Similarly, results from Analysis 2 are summarised in
Table 4.
Table 4:Observed and expected numbers of detected photoelectrons
for the various radiator and filter configurations determined using
Analysis 2. The final column indicates the mean of the two analyses
for the ratio of Observed/Predicted numbers of photoelectrons.
Layout
Observed
Observed
Mean
Predicted
(Anal. 1 & 2)
1
5.06
0.88
0.89
2
7.15
1.01
1.02
3
12.42
1.10
1.08
4
1.85
1.39
1.42
5
1.80
0.67
0.70
6
1.18
0.95
0.94
7
1.45
0.90
0.77
8
0.83
1.15
1.12
Due to differences in the numbers of pixels used and in the pedestal
selection between the two analyses, it is not possible to compare
directly the raw numbers of observed photons for each layout.
Instead, the combined ratio of number of photons observed to that
predicted is averaged for the two methods and are given in the final
column of Table 4.
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