Feasibility study for the development of multilayered solar cells for proton linear energy transfer depth profile measurement

Author:

Jeong Seonghoon1,Kim Chae‐Eon23,Kim Chankyu2,Pak Sang‐il2,An Seohyeon24,Cheon Wonjoong5,Shin Dongho2,Lim Young Kyung2,Jeong Jong Hwi2,Kim Haksoo2,Chung Yoonsun3,Choi Sang Hyoun6,Lee Se Byeong2

Affiliation:

1. Department of Neurosurgery College of Medicine Ilsan Paik Hospital Inje University Goyang Republic of Korea

2. Proton Therapy Center National Cancer Center Goyang Republic of Korea

3. Department of Nuclear Engineering Hanyang University Seoul Republic of Korea

4. Department of Physics Hanyang University Seoul Republic of Korea

5. Department of Radiation Oncology Seoul St. Mary's Hospital College of Medicine The Catholic University of Korea Seoul Republic of Korea

6. Radiation Therapy Technology and Standards Korea Institute of Radiological & Medical Sciences Seoul Republic of Korea

Abstract

AbstractBackgroundPrevious study proposed a method to measure linear energy transfer (LET) at specific points using the quenching magnitude of thin film solar cells. This study was conducted to propose a more advanced method for measuring the LET distribution.PurposeThis study focuses on evaluating the feasibility of estimating the proton LET distribution in proton therapy. The feasibility of measuring the proton LET and dose distribution simultaneously using a single‐channel configuration comprising two solar cells with distinct quenching constants is investigated with the objective of paving the way for enhanced proton therapy dosimetry.MethodsTwo solar cells with different quenching constants were used to estimate the proton LET distribution. Detector characteristics (e.g., dose linearity and dose‐rate dependency) of the solar cells were evaluated to assess their suitability for dosimetry applications. First, using a reference beam condition, the quenching constants of the two solar cells were determined according to the modified Birks equation. The signal ratios of the two solar cells were then evaluated according to proton LET in relation to the estimated quenching constants. The proton LET distributions of six test beams were obtained by measuring the signal ratios of the two solar cells at each depth, and the ratios were evaluated by comparing them with those calculated by Monte Carlo simulation.ResultsThe detector characterization of the two solar cells including dose linearity and dose‐rate dependence affirmed their suitability for use in dosimetry applications. The maximum difference between the LET measured using the two solar cells and that calculated by Monte Carlo simulation was 2.34 keV/µm. In the case of the dose distribution measured using the method proposed in this study, the maximum difference between range measured using the proposed method and that measured using a multilayered ionization chamber was 0.7 mm. The expected accuracy of simultaneous LET and dose distribution measurement using the method proposed in this study were estimated to be 3.82%. The signal ratios of the two solar cells, which are related to quenching constants, demonstrated the feasibility of measuring LET and dose distribution simultaneously.ConclusionThe feasibility of measuring proton LET and dose distribution simultaneously using two solar cells with different quenching constants was demonstrated. Although the method proposed in this study was evaluated using a single channel by varying the measuring depth, the results suggest that the proton LET and dose distribution can be simultaneously measured if the detector is configured in a multichannel form. We believe that the results presented in this study provide the envisioned transition to a multichannel configuration, with the promise of substantially advancing proton therapy's accuracy and efficacy in cancer treatment.

Funder

National Research Council of Science and Technology

Publisher

Wiley

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