Comisión Nacional de Energía Atómica, Av. del Libertador 8250, Ciudad de Buenos Aires 1429, Argentina.
Med Phys. 2011 Dec;38(12):6502-12. doi: 10.1118/1.3660204.
A rhodium self-powered neutron detector (Rh SPND) has been specifically developed by the Comisión Nacional de Energía Atómica (CNEA) of Argentina to measure locally and in real time thermal neutron fluxes in patients treated with boron neutron capture therapy (BNCT). In this work, the thermal and epithermal neutron response of the Rh SPND was evaluated by studying the detector response to two different reactor spectra. In addition, during clinical trials of the BNCT Project of the CNEA, on-line neutron flux measurements using the specially designed detector were assessed.
The first calibration of the detector was done with the well-thermalized neutron spectrum of the CNEA RA-3 reactor thermal column. For this purpose, the reactor spectrum was approximated by a Maxwell-Boltzmann distribution in the thermal energy range. The second calibration was done at different positions along the central axis of a water-filled cylindrical phantom, placed in the mixed thermal-epithermal neutron beam of CNEA RA-6 reactor. In this latter case, the RA-6 neutron spectrum had been well characterized by both calculation and measurement, and it presented some marked differences with the ideal spectrum considered for SPND calibrations at RA-3. In addition, the RA-6 neutron spectrum varied with depth in the water phantom and thus the percentage of the epithermal contribution to the total neutron flux changed at each measurement location. Local (one point-position) and global (several points-positions) and thermal and mixed-field thermal neutron sensitivities were determined from these measurements. Thermal neutron flux was also measured during BNCT clinical trials within the irradiation fields incident on the patients. In order to achieve this, the detector was placed on patient's skin at dosimetric reference points for each one of the fields. System stability was adequate for this kind of measurement.
Local mixed-field thermal neutron sensitivities and global thermal and mixed-field thermal neutron sensitivities derived from measurements performed at the RA-6 were compared and no significant differences were found. Global RA-6-based thermal neutron sensitivity showed agreement with pure thermal neutron sensitivity measurements performed in the RA-3 spectrum. Additionally, the detector response proved nearly unchanged by differences in neutron spectra from real (RA-6 BNCT beam) and ideal (considered for calibration calculations at RA-3) neutron source descriptions. The results confirm that the special design of the Rh SPND can be considered as having a pure thermal response for neutron spectra with epithermal-to-thermal flux ratios up to 12%. In addition, the linear response of the detector to thermal flux allows the use of a mixed-field thermal neutron sensitivity of 1.95 ± 0.05 × 10(-21) A n(-1)[middle dot]cm² [middle dot]s. This sensitivity can be used in spectra with up to 21% epithermal-to-thermal flux ratio without significant error due to epithermal neutron and gamma induced effects. The values of the measured fluxes in clinical applications had discrepancies with calculated results that were in the range of -25% to +30%, which shows the importance of a local on-line independent measurement as part of a treatment planning quality control system.
The usefulness of the CNEA Rh SPND for the on-line local measurement of thermal neutron flux on BNCT patients has been demonstrated based on an appropriate neutron spectra calibration and clinical applications.
阿根廷国家原子能委员会(CNEA)专门开发了一种铑自供电中子探测器(Rh SPND),用于测量硼中子俘获治疗(BNCT)患者中局部实时热中子通量。在这项工作中,通过研究探测器对两种不同反应堆光谱的响应,评估了 Rh SPND 的热中子和超热中子响应。此外,在 CNEA BNCT 项目的临床测试期间,使用专门设计的探测器进行了在线中子通量测量。
探测器的第一次校准是在 CNEA RA-3 反应堆热柱的充分热化中子谱下进行的。为此,将反应堆光谱在热能范围内近似为麦克斯韦-玻尔兹曼分布。第二次校准是在位于 CNEA RA-6 反应堆混合热-超热中子束中的充满水的圆柱形幻影的中心轴的不同位置进行的。在后一种情况下,RA-6 中子谱已经通过计算和测量得到了很好的表征,并且与 RA-3 中用于 SPND 校准的理想谱相比,它具有一些明显的差异。此外,RA-6 中子谱随水幻境内的深度而变化,因此在每个测量位置处总中子通量的超热贡献百分比发生变化。从这些测量中确定了局部(一个点位置)和全局(多个点位置)以及热和混合场热中子灵敏度。在 BNCT 临床测试期间,还在入射到患者的照射场内在线测量了热中子通量。为此,将探测器放置在每个场的患者皮肤的剂量参考点上。这种测量的系统稳定性足够。
比较了在 RA-6 上进行的测量得出的局部混合场热中子灵敏度和全局热和混合场热中子灵敏度,未发现显著差异。基于 RA-6 的全局热中子灵敏度与在 RA-3 光谱中进行的纯热中子灵敏度测量结果一致。此外,探测器的响应证明几乎不受来自真实(RA-6 BNCT 束)和理想(用于 RA-3 校准计算)中子源描述的中子谱的差异的影响。结果证实,对于超热通量与热通量之比高达 12%的中子谱,特殊设计的 Rh SPND 可被视为具有纯热响应。此外,探测器对热通量的线性响应允许使用 1.95±0.05×10(-21)A n(-1)[中圆点]cm² [中圆点]s 的混合场热中子灵敏度。在不超过 21%的超热-热通量比的光谱中,可以使用此灵敏度,而不会因超热中子和伽马诱导效应而产生显著误差。临床应用中测量的通量值与计算结果相差在-25%至+30%之间,这表明作为治疗计划质量控制系统的一部分,进行局部在线独立测量非常重要。
基于适当的中子光谱校准和临床应用,证明了 CNEA Rh SPND 可用于 BNCT 患者的在线局部热中子通量测量。