High-resolution entry and exit surface dosimetry in a 1.5 T MR-linac

被引:6
作者
Patterson, E. [1 ]
Stokes, P. [4 ]
Cutajar, D. [1 ]
Rosenfeld, A. [1 ,2 ]
Baines, J. [4 ,5 ]
Metcalfe, P. [1 ,2 ,3 ]
Powers, M. [4 ,5 ]
机构
[1] Univ Wollongong, Ctr Med & Radiat Phys, Wollongong, NSW, Australia
[2] Univ Wollongong, Illawarra Hlth Med Res Inst, Wollongong, NSW, Australia
[3] Ingham Inst Appl Med Res, Liverpool, NSW, Australia
[4] Townsville Hosp, Townsville Canc Ctr, Hlth Serv, Townsville, Qld, Australia
[5] James Cook Univ, Coll Sci & Engn, Townsville, Qld, Australia
关键词
MR-linac; Elekta Unity; MOSFET; Skin dose; Surface dosimetry; Monte Carlo; MV RADIOTHERAPY ACCELERATOR; SKIN DOSE MEASUREMENT; IN-VIVO DOSIMETRY; MAGNETIC-FIELD; MOSKIN DETECTOR; TLD EXTRAPOLATION; SCANNER; BEAM; ORIENTATION; ENTRANCE;
D O I
10.1007/s13246-023-01251-6
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
The magnetic field of a transverse MR-linac alters electron trajectories as the photon beam transits through materials, causing lower doses at flat entry surfaces and increased doses at flat beam-exiting surfaces. This study investigated the response of a MOSFET detector, known as the MOSkin (TM), for high-resolution surface and near-surface percentage depth dose measurements on an Elekta Unity. Simulations with Geant4 and the Monaco treatment planning system (TPS), and EBT-3 film measurements, were also performed for comparison. Measured MOSkin (TM) entry surface doses, relative to D-max, were (9.9 +/- 0.2)%, (10.1 +/- 0.3)%, (11.3 +/- 0.6)%, (12.9 +/- 1.0)%, and (13.4 +/- 1.0)% for 1 x 1 cm(2), 3 x 3 cm(2), 5 x 5 cm(2), 10 x 10 cm(2), and 22 x 22 cm(2) fields, respectively. For the investigated fields, the maximum percent differences of Geant4, TPS, and film doses extrapolated and interpolated to a depth suitable for skin dose assessment at the beam entry, relative to MOSkin (TM) measurements at an equivalent depth were 1.0%, 2.8%, and 14.3%, respectively, and at a WED of 199.67 mm at the beam exit, 3.2%, 3.7% and 5.7%, respectively. The largest measured increase in exit dose, due to the electron return effect, was 15.4% for the 10 x 10 cm(2) field size using the MOSkin (TM) and 17.9% for the 22 x 22 cm(2) field size, using Geant4 calculations. The results presented in the study validate the suitability of the MOSkin (TM) detector for transverse MR-linac surface dosimetry.
引用
收藏
页码:787 / 800
页数:14
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