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基于加速器的近阈能7Li(p,n)7Be硼中子俘获治疗中锂靶厚度和质子能量稳定性的变化

Variations in lithium target thickness and proton energy stability for the near-threshold 7Li(p,n)7Be accelerator-based BNCT.

作者信息

Kobayashi Tooru, Bengua Gerard, Tanaka Kenichi, Nakagawa Yoshinobu

机构信息

Kyoto University Research Reactor Institute, Osaka, Japan. Nuclear Engineering Department, Kyoto University, Kyoto, Japan.

出版信息

Phys Med Biol. 2007 Feb 7;52(3):645-58. doi: 10.1088/0031-9155/52/3/008. Epub 2007 Jan 10.

Abstract

The usable range of thickness for the solid lithium target in the accelerator-based neutron production for BNCT via the near-threshold (7)Li(p,n)(7)Be reaction was investigated. While the feasibility of using a (7)Li-target with thickness equal to that which is required to slow down a mono-energetic 1.900 MeV incident proton to the 1.881 MeV threshold of the (7)Li(p,n)(7)Be reaction (i.e., t(min) = 2.33 microm) has already been demonstrated, dosimetric properties of neutron fields from targets greater than t(min) were assessed as thicker targets would last longer and offer more stable neutron production. Additionally, the characteristics of neutron fields generated by (7)Li(p,n)(7)Be for Gaussian incident protons with mean energy of 1.900 MeV were evaluated at a (7)Li-target thickness t(min). The main evaluation index applied in this study was the treatable protocol depth (TPD) which corresponds to the depth in an irradiated medium that satisfies the requirements of the adapted dose protocol. A maximum TPD (TPD(max)) was obtained for each irradiation condition from the relationship between the TPD and the thickness of boron dose enhancer (BDE) used. For a mono-energetic 1.900 MeV proton beam, the deepest TPD(max) of 3.88 cm was attained at the (7)Li-target thickness of t(min) and a polyethylene BDE of 1.10 cm. When the intended TPD for a BNCT clinical treatment is shallower than the deepest TPD(max), the usable (7)Li-target thickness would be between t(min) and an upper limit t(upper) whose value depends on the BDE thickness used. In terms of the effect of stability of the incident proton energy, Gaussian incident proton energies stable to within +/-10 keV of 1.900 MeV were found to be feasible for the neutron production via the near-threshold (7)Li(p,n)(7)Be reaction for BNCT provided that a suitable BDE is used.

摘要

研究了基于加速器的硼中子俘获治疗(BNCT)中,通过近阈(7)Li(p,n)(7)Be反应产生中子时,固体锂靶的可用厚度范围。虽然已经证明了使用厚度等于将单能1.900 MeV入射质子减速到(7)Li(p,n)(7)Be反应的1.881 MeV阈值所需厚度的(7)Li靶的可行性(即t(min)= 2.33微米),但由于较厚的靶持续时间更长且能提供更稳定的中子产生,因此评估了厚度大于t(min)的靶产生的中子场的剂量学特性。此外,在(7)Li靶厚度t(min)下,评估了由平均能量为1.900 MeV的高斯入射质子通过(7)Li(p,n)(7)Be产生的中子场的特性。本研究中应用的主要评估指标是可治疗方案深度(TPD),它对应于满足适配剂量方案要求的辐照介质中的深度。根据TPD与所用硼剂量增强剂(BDE)厚度之间的关系,为每种辐照条件获得了最大TPD(TPD(max))。对于单能1.900 MeV质子束,在(7)Li靶厚度为t(min)且聚乙烯BDE为1.10 cm时,获得了3.88 cm的最深TPD(max)。当BNCT临床治疗的预期TPD比最深TPD(max)浅时,可用的(7)Li靶厚度将在t(min)和上限t(upper)之间,其值取决于所用BDE的厚度。就入射质子能量稳定性的影响而言,发现对于BNCT通过近阈(7)Li(p,n)(7)Be反应产生中子,如果使用合适的BDE,高斯入射质子能量在1.900 MeV的+/-10 keV范围内稳定是可行的。

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