Monte Carlo calculation of quality correction factors based on air kerma and absorbed dose to water in medium energy x-ray beams

被引:3
|
作者
Czarnecki, Damian [1 ]
Zink, Klemens [1 ,4 ]
Pimpinella, Maria [2 ]
Borbinha, Jorge [3 ]
Teles, Pedro [5 ]
Pinto, Massimo [2 ]
机构
[1] Univ Appl Sci Giessen THM, Inst Med Phys & Radiat Protect, Giessen, Germany
[2] Ist Nazl Metrol Radiaz Ionizzanti ENEA INMRI, Rome, Italy
[3] Inst Super Tecn IST, Ctr Ciencias & Tecnol Nucl, Bobadela, Portugal
[4] Univ Med Ctr Giessen & Marburg, Dept Radiotherapy & Radiat Oncol, Marburg, Germany
[5] Univ Porto, Dept Fis & Astron, Fac Ciencias, Porto, Portugal
来源
PHYSICS IN MEDICINE AND BIOLOGY | 2020年 / 65卷 / 24期
关键词
medium energy x-rays; dosimetry; Monte Carlo simulations; IAEA TRS-398; CALORIMETER;
D O I
10.1088/1361-6560/abc5c9
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
Clinical dosimetry is typically performed using ion chambers calibrated in terms of absorbed dose to water. As primary measurement standards for this quantity for low and medium energy x-rays are available only since a few years, most dosimetry protocols for this photon energy range are still based on air kerma calibration. For that reason, data for beam quality correction factors k(Q,Q0), necessary for the application of dose to water based protocols, are scarce in literature. Currently the international IAEA TRS-398 Code of Practice is under revision and new k(Q,Q0) factors for a large number of ion chambers will be introduced in the update of this protocol. Several international groups provided the IAEA with experimental and Monte Carlo based data for this revision. Within the European Community the EURAMET 16NRM03 RTNORM project was initiated for that purpose. In the present study, Monte Carlo based results for the beam quality correction factors in medium energy x-ray beams for six ion chambers applying different Monte Carlo codes are presented. Additionally, the perturbation factor p(Q), necessary for the calculation of dose to water from an air kerma calibration coefficient, was determined. The beam quality correction factor k(Q,Q0) for the chambers varied in the investigated energy range by about 4%-5%, and for five out of six chambers the data could be fitted by a simple logarithmic function, if the half-value-layer was used as the beam quality specifier. Corresponding data using different Monte Carlo codes for the same ion chamber agreed within 0.5%. For the perturbation factor p(Q), the data did not obey a comparable simple relationship with the beam quality specifier. The variation of p(Q) for all ion chambers was in the range of 3%-4%. Compared to recently published data, our p(Q) data is around 1% larger, although the same Monte Carlo code has been used. Compared to the latest experimental data, there are even deviations in the range of 2%.
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页数:14
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