Surface and near-surface dose measurements at beam entry and exit in a 1.5 T MR-Linac using optically stimulated luminescence dosimeters.

Phys Med Biol

Sunnybrook Health Sciences Centre/Odette Cancer Centre, 2075 Bayview Ave, Toronto, ON M4N 3M5, Canada. Faculty of Medicine, Department of Radiation Oncology, University of Toronto, 149 College Street, Suite 504, Toronto, Ontario M5T 1P5, Canada. Sunnybrook Health Sciences Centre, 2075 Bayview Avenue Toronto, ON M4N 3M5 Ontario, Canada. Author to whom any correspondence should be addressed.

Published: February 2020

The objective of this study is to measure surface and near-surface dose at entry and exit surfaces in a 1.5 T MR-Linac (Elekta AB, Stockholm, Sweden) using optically stimulated luminescence dosimeters (OSLDs). OSLDs were expected to be useful for measuring surface dose in a strong magnetic field because they can be taped to undersides to measure exit dose, and their dose response have been shown to be reasonably insensitive to variations in beam angle, beam energy, and magnetic fields. The surface and near-surface dose at the entry and exit of a 20 cm thick solid water phantom was measured with OSLDs for 5  ×  5, 10  ×  10, and 22  ×  22 cm field sizes. The solid water phantom was elevated off the couch top to produce an air gap of 3.7 cm so as to observe the electron return effect (ERE) near the beam exit surface. Measurement depths ranged from surface to 15 mm deep from entry and exit surfaces. The phantom dose distribution was also computed in the Monaco (Elekta AB, Stockholm, Sweden) Monte Carlo treatment planning system (TPS). For the 5  ×  5, 10  ×  10, and 22  ×  22 cm field sizes the surface dose at depth 0 mm was extrapolated from OSLD measurements to be 10.9%, 12.0%, and 13.5%. The surface entry dose was found to be far less field size-dependent compared to a conventional linac, likely due to a lack of electronic contamination due to the strong magnetic field perpendicular to the beam. The ERE effect was observed in the measurements near the exit surface of the phantom, and was in close agreement with the TPS calculation.

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http://dx.doi.org/10.1088/1361-6560/ab64b6DOI Listing

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