Graduate School of Comprehensive Human Sciences, University of Tsukuba, 1-1-1, Tennodai, Tsukuba, Ibaraki 305-8577, Japan.
Medipolis Proton Therapy and Research Center, 4423, Higashikata, Ibusuki, Kagoshima 891-0403, Japan.
Phys Med Biol. 2024 Oct 21;69(21). doi: 10.1088/1361-6560/ad8546.
The linear energy transfer (LET) of proton therapy beams increases rapidly from the Bragg peak to the end of the beam. Although the LET can be determined using analytical or computational methods, a technique for efficiently measuring its spatial distribution has not yet been established. Thus, the purpose of this study is to develop a technique to measure the two-dimensional LET distribution in proton therapy in real time using a combination of multiple scintillators with different quenching.Inorganic and organic scintillator sheets were layered and irradiated with proton beams. Two-color signals of the CMOS sensor were obtained from the scintillation light and calibration curves were generated using LET. LET was calculated using Monte Carlo simulations asLETtandLETdweighted by fluence and dose, respectively. The accuracy of the calibration curve was evaluated by comparing the calculated and measured LET values for the 200 MeV monoenergetic and spread-out Bragg peak (SOBP) beams. LET distributions were obtained from the calibration curves.The deviation between the calculated and measured LET values was evaluated. For bothLETtandLETd, the deviation in the plateau region of the monoenergetic and SOBP beams tended to be larger than those in the peak region. The deviation was smaller forLETd. In the obtainedLETddistribution, the deviation between the calculated and measured values agreed within 3% in the peak region, while the deviation was larger in other regions.The LET distribution can be measured with a single irradiation using two scintillator sheets. This method may be effective for verifying LET in daily clinical practice and for quality control.
线性能量转移(LET)质子治疗束从布拉格峰到束末端迅速增加。虽然 LET 可以使用分析或计算方法来确定,但尚未建立一种有效测量其空间分布的技术。因此,本研究的目的是开发一种使用具有不同猝灭的多个闪烁体组合实时测量质子治疗中二维 LET 分布的技术。无机和有机闪烁体片被分层并受到质子束照射。从闪烁光获得 CMOS 传感器的双色信号,并使用 LET 生成校准曲线。使用 Monte Carlo 模拟计算 LET,分别用剂量和剂量加权的 LETt 和 LETd。通过比较单能和扩展布拉格峰(SOBP)束的计算和测量 LET 值来评估校准曲线的准确性。从校准曲线获得 LET 分布。评估计算和测量 LET 值之间的偏差。对于 LETt 和 LETd,单能和 SOBP 束的平台区域的偏差倾向于比峰值区域的偏差大。LETd 的偏差较小。在获得的 LETd 分布中,峰值区域内计算值和测量值之间的偏差在 3%以内,而在其他区域偏差较大。可以使用两个闪烁体片进行单次照射来测量 LET 分布。这种方法可能有助于在日常临床实践中验证 LET,并进行质量控制。