31
The
𝐸
𝑙𝑜𝑠𝑠
for each sample was determined using the SRIM simulations discussed
previously. The mass was determined for the irradiated spot area (1.8 mm x 1.8
mm), using the densities given by the manufacturers
and accounting for each
sample’s thickness.
The number of protons impinging the sample,
was determined using the
relationship
𝑁
𝑝
=
𝑖𝑡
𝑞
, where
i
is the current of the proton beam used,
t
is the total
irradiation time and
q
is the charge of a proton. The total charge passed through
each sample for their respective exposure times during irradiation was used for
the calculations. Appendix B contains the
tables summarising the beam
conditions and calculated doses, as well as beam current distribution plots for all
samples.
4.2.
Overview of the techniques used to analyse
damage
The effects of proton damage on the optical properties
of the samples were
characterised by conducting light transmission, light
yield and fluorescence
studies. Whilst the technique of Raman sp ectroscopy was used to investigate the
structural damage undergone by the scintillators.
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