25
Figure 4-2: Plot of the range over which protons stop within the PVT and PS targets.
Simulations of 6 MeV protons through targets of 300 -400 μm thickness were then
conducted in order to establish the energy of particles transmitted f rom the target.
This was used in order to estimate the amount of energy deposited by a 6 MeV
proton traversing the samples, which was a parameter needed for estimating the
absorbed dose upon irradiation of the samples. For a 6
MeV proton traversing
through
a PVT based scintillator, the estimated amount
of energy deposited is
3.20 MeV through a 350 μm thick sample and 3.89 MeV through a 400 μm thick
sample.
4.1.2.
Sample preparation
Samples were prepared with targeted dimensions of 5 mm x 5 mm area and 350
μm thickness. Since cutting the samples caused them to become rough and
opaque, samples were polished to improve their transparency. A polishing
procedure based on standard metallographic techniques [27] was employed.
A “Buehler IsoMet” low speed cut-off machine was used to section rectangular
bars of 5 mm x 5 mm area and with varying lengths. The lengths depended on the
dimensions of the sample blocks provided by the manufacturers. The bars were
further cut along their cross-section into 1 mm thick slices.
26
The cutting operation was carried out using a diamond finished blade with cutting
fluid as a lubricant. Photographs of the Buehler
IsoMet cutting machine are
shown in Figure 4-3.
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