Figure 5-6: 2D mapping of the PMT signal with Sr90 source position, indicating signal regions corresponding to regions on the experimental set -up. The beta electrons emitted by the source can interact over a 2 mm lateral radius
from the actual position of the source. Hence the signal obtained for the 1 mm
diameter fiber spans over ~5 mm. This is similarly observed over the sample
region. Since samples were tested after irradiation only, the intention was to
compute the ratio of light loss by taking the ratio between the signal over the
irradiated spot region and an un-irradiated “corner region” of the same sample.
This however was not an accurate measure due to the large range of the
interaction of the source. Thus, a control un-irradiated sample for each
scintillator type had to be tested as well so that a comparison of the loss could be
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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
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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.