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LIFE01200604005 Shri Somnath Ghosh - Homi Bhabha National ...

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CHAPTER 2<br />

MATERIALS AND METHODS<br />

primary proton beam from the FOTIA was collimated using an adjustable slit to reduce the<br />

fluence and then diffused using a gold foil. The diffused beam was channeled to the exit window<br />

made of 20 micrometer titanium foil of 3 cm diameter to get uniformly distributed irradiation<br />

area. The samples were thus irradiated under normal atmospheric pressure at 24 o C. The target to<br />

be irradiated was positioned at a distance of 11 mm from the exit window, that being the closest<br />

possible place to mount the target. Before the irradiation, a silicon surface barrier (SSB) detector<br />

was positioned at the same position where samples were irradiated and the beam energy as well<br />

as the uniformity was measured. Another SSB detector placed inside the scattering chamber at a<br />

forward angle of 40 o to the primary beam, after the gold foil, served as a monitor detector. The<br />

ratio of the monitor detector counts to that of the flux measured using SSB detector at the sample<br />

position was measured by multiple trials and the calibration factor was obtained. Monitor<br />

detector counts and the measured ratio were used for delivering the required fluence to the<br />

samples. Flux was calculated to be 10 8 and the fluence was kept such that each cell is hit by at<br />

least 100 proton particles ensuring that bystander effect is kept to minimum. Fluence was then<br />

used to calculate dose with the help of specific ionization curve constructed for the given energy<br />

distribution and composition of the cellline. The average energy of the proton beam used in this<br />

study was measured to be 3.2 MeV and corresponding estimated LET is 12.5 keV/µm within the<br />

cell layer. Initial portion of Bragg’s curve was used for dose estimation since the cell layer used<br />

for irradiation was in monolayer geometry with thickness less than 10µm, which helped to avoid<br />

steep increase in LET within the sample.<br />

The cells were grown in monolayer geometry on 35mm petri dishes. Media was removed and<br />

petridishes were mounted on the exit window vertically for the irradiation, after which they were<br />

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