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made. Figure 5-7 shows 3D mappings indicating loss to the light yield signal for
different irradiation doses of EJ200 samples. Photographs of the sample
indicating where the corresponding spot regions occur are also shown.
Figure 5-7: 3D mappings of the light yield for several EJ200 samples with different levels
of proton induced radiation damage.
Three measurements were taken for each sample, with the sample rotated in the
holder for each measurement. It was observed that
the geometry of the sample
tested played a large impact on the magnitude of the PMT signal measured. This
is because the amount of light transferred between the scintillator and the fiber
is dependent on the contact made between the two.
Thicker samples therefore
make a better contact and result in a larger measured signal. The different
samples also varied slightly in their size, with edge lengths varying by up to 0.3
45
mm. This further impacted on the signal measured.
A comparison betwe en the
potential systematic variations and their impact on the three measured signals
tested per sample is drawn in Figure 5-8 for all the TileCal samples tested.
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