LET measurements in proton and helium-ion beams of therapeutic energies using a silicon pixel detector towards a tool for quality assurance

IF 3.2 2区 医学 Q1 RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING
Medical physics Pub Date : 2025-09-04 DOI:10.1002/mp.18085
Yasmin Hamad, Ferisya Kusuma Sari, Renato Félix-Bautista, Mária Martišíková, Andrea Mairani, Tim Gehrke
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引用次数: 0

Abstract

Background

As advanced treatment plans increasingly include optimizing both dose and linear energy transfer (LET), there is a growing demand for tools to measure LET in clinical settings. Although various detection systems have been investigated in this pursuit, the scarcity of detectors capable of providing per-ion data for a fast and streamlined verification of LET distributions remains an issue. Silicon pixel detector technology bridges this gap by enabling rapid tracking of single-ion energy deposition.

Purpose

This study proposes a methodology for assessing LET and relative biological effectiveness (RBE) in mixed radiation fields produced by clinical proton and helium ion beams, using a hybrid silicon pixel detector equipped with a Timepix3 chip.

Methods

The Timepix3 detector was placed behind PMMA slabs of different thicknesses and exposed to initially monoenergetic proton and helium-ion beams. The detector featured a 300 µm-thick silicon sensor operated in partial depletion. Silicon-based LET spectra were derived from single-ion deposited energy across the sensor and subsequently converted to water-equivalent spectra. Track- and dose-averaged LET (LETt and LETd) were calculated from these spectra. LET measurements were used as input to estimate the RBE via the modified microdosimetric kinetic model (mMKM) assuming an (α/β)γ value of 2 Gy. Measurements were compared with simulations performed using the FLUKA Monte Carlo code. Energy deposition spectra, LETt and LETd values were simulated at various depths in PMMA for the radiation fields used, by considering the contribution from the secondary particles generated in the ion interaction processes as well.

Results

Energy deposition spectra were validated against Monte Carlo simulations, showing good agreement in both spectral shapes and positions. However, a depth uncertainty of less than 1 mm and other potential differences between measurements and simulations led to deviations, particularly in the distal region of the Bragg curve. Relative differences of LETd between measurements and simulations were within 3% for protons and 10% for helium ions upstream of the Bragg curves. Notably, larger discrepancies were observed in the distal part of the Bragg curve, with maximum relative differences of 7% for protons and 17% for helium ions. Average differences between RBE predictions from measured and simulated LET spectra were within 1% and 6% for protons and helium, respectively. Nevertheless, for both particle types, most measurements agreed with simulations within 1σ experimental uncertainty across the measured depths, with deviations beyond 1σ generally remaining within 3σ.

Conclusions

This study demonstrates the performance of silicon pixel detectors with respect to LET measurements and RBE estimation in clinical proton and helium-ion beams. The streamlined and accessible outline of the proposed methodology supports easy implementation into clinical routines, promising a viable and sound quality assurance tool for particle therapy.

Abstract Image

Abstract Image

Abstract Image

利用硅像素探测器对质子和氦离子束治疗能量进行LET测量,成为质量保证工具
随着高级治疗计划越来越多地包括优化剂量和线性能量转移(LET),对临床环境中测量LET的工具的需求日益增长。尽管在这方面已经研究了各种检测系统,但能够为LET分布的快速和精简验证提供每离子数据的检测器的稀缺性仍然是一个问题。硅像素探测器技术通过实现单离子能量沉积的快速跟踪弥补了这一差距。本研究提出了一种利用配备Timepix3芯片的混合硅像元探测器评估临床质子和氦离子束混合辐射场LET和相对生物有效性(RBE)的方法。方法将Timepix3探测器置于不同厚度的PMMA板后,初始暴露于单能质子和氦离子束下。该探测器具有300微米厚的硅传感器,在部分耗尽中工作。硅基LET光谱来源于传感器上的单离子沉积能量,随后转换为水等效光谱。根据这些光谱计算了径迹和剂量平均LET (LETt和LETd)。假设(α/β)γ值为2 Gy,利用LET测量值作为输入,通过改进的微剂量动力学模型(mMKM)估计RBE。测量结果与使用FLUKA蒙特卡罗代码进行的模拟结果进行了比较。通过考虑离子相互作用过程中产生的二次粒子的贡献,模拟了所使用的PMMA辐射场在不同深度下的能量沉积谱、LETt和LETd值。结果对能量沉积谱进行了蒙特卡罗模拟验证,在光谱形状和位置上都表现出较好的一致性。然而,小于1毫米的深度不确定性以及测量和模拟之间的其他潜在差异导致了偏差,特别是在布拉格曲线的远端区域。测量值与模拟值之间的相对差值在布拉格曲线上游的质子为3%,氦离子为10%。值得注意的是,在布拉格曲线的远端观察到更大的差异,质子和氦离子的最大相对差异为7%和17%。质子和氦的测量和模拟LET光谱的RBE预测之间的平均差异分别在1%和6%以内。然而,对于这两种粒子类型,大多数测量结果与模拟结果在测量深度的1σ实验不确定度内一致,超过1σ的偏差通常保持在3σ以内。结论本研究证明了硅像素探测器在质子和氦离子束的LET测量和RBE估计方面的性能。所提出的方法的简化和易于访问的大纲支持易于实施到临床常规,有望为粒子治疗提供可行和健全的质量保证工具。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Medical physics
Medical physics 医学-核医学
CiteScore
6.80
自引率
15.80%
发文量
660
审稿时长
1.7 months
期刊介绍: Medical Physics publishes original, high impact physics, imaging science, and engineering research that advances patient diagnosis and therapy through contributions in 1) Basic science developments with high potential for clinical translation 2) Clinical applications of cutting edge engineering and physics innovations 3) Broadly applicable and innovative clinical physics developments Medical Physics is a journal of global scope and reach. By publishing in Medical Physics your research will reach an international, multidisciplinary audience including practicing medical physicists as well as physics- and engineering based translational scientists. We work closely with authors of promising articles to improve their quality.
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