2021
DOI: 10.1002/mp.15244
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Feasibility of operating a millimeter‐scale graphite calorimeter for absolute dosimetry of small‐field photon beams in the clinic

Abstract: To characterize and build a cylindrically layered graphite calorimeter the size of a thimble ionization chamber for absolute dosimetry of small fields. This detector has been designed in a familiar probe format to facilitate integration into the clinical workflow. The feasibility of operating this absorbed dose calorimeter in quasi-adiabatic mode is assessed for high-energy acceleratorbased photon beams. Methods: This detector, herein referred to as Aerrow MK7, is a miniaturized version of a previously validat… Show more

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Cited by 2 publications
(4 citation statements)
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“…The Monte Carlo dose ratio from Equation () was calculated to be 1.149(4) and was compared to the water‐to‐graphite stopping power ratio (SPR = 1.137(9)), a difference of 1.2(1)%. The difference in the two values is due to the volume averaging due to the non‐homogeneity of the beam and the radiation field perturbation caused by the detector 16 . The volume averaging can be roughly estimated to be 2.8% for the beam setup, which has a Gaussian shape with an FWHM of about 80 mm.…”
Section: Resultsmentioning
confidence: 99%
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“…The Monte Carlo dose ratio from Equation () was calculated to be 1.149(4) and was compared to the water‐to‐graphite stopping power ratio (SPR = 1.137(9)), a difference of 1.2(1)%. The difference in the two values is due to the volume averaging due to the non‐homogeneity of the beam and the radiation field perturbation caused by the detector 16 . The volume averaging can be roughly estimated to be 2.8% for the beam setup, which has a Gaussian shape with an FWHM of about 80 mm.…”
Section: Resultsmentioning
confidence: 99%
“…The difference in the two values is due to the volume averaging due to the non-homogeneity of the beam and the radiation field perturbation caused by the detector. 16 The volume averaging can be roughly estimated to be 2.8% for the beam setup, which has a Gaussian shape with an FWHM of about 80 mm. Therefore, it can be estimated that the net perturbation from the presence of the detector would be on the order of 4%.…”
Section: Dose Per Pulsementioning
confidence: 97%
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