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simulates the experimental setup and conditions for evaluating manunography X-ray beamradiation dose. Presented in Chapter 6 is the simulation work using the PENELOPE MC code.1.5.4. Overview of Dosimetry with DiamondDiamond is a unique element with attractive physical properties such as wide band gapmaking it an excellent insulator, wide transmission band, optically transparent, high chargecarrier mobility, high breakdown voltage, high thermal conductivity and low thermalexpansion coefficient, small dielectric constant, excellent radiation hardness, physically hardand chemically inert. The near tissue equivalence and chemical inertness of diamond havebeen identified to be important in both medical physics and health physics as a radiationmonitoring tool (Nam et al., 1987). Thus, as a radiation dosimeter, it does not require largecorrection factors to convert the response to a true deposited radiation dose. This is becausethe energy response or energy absorption of diamond as a dose-sensing element per unitexposure will be similar to that oftissue.Diamond also has low noise contribution arising from leakage currents due to the large bandgap. Further, good sensitivity compared to ionization chambers has been found (Bruzzi et aI.,2000) and the insensitivity to radiation damage makes diamond a material more suitable thanmost solid-state detectors currently being used for on-line dosimetric applications (Plankskoy,1980; Rustgi, 1995).The applications of synthetic diamond crystal as radiation sensing elements have beenconcentrated mainly on its response to charge particles. These applications have been both innuclear and medical physics. Some ofthe studies include: (Burgemeister, 198I) rate ionization18

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