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用于中子俘获治疗的厚铍靶作为超热中子源。

Thick beryllium target as an epithermal neutron source for neutron capture therapy.

作者信息

Wang C K, Moore B R

机构信息

Nuclear Engineering & Health Physics Program, Georgia Institute of Technology, Atlanta 30332-0225.

出版信息

Med Phys. 1994 Oct;21(10):1633-8. doi: 10.1118/1.597269.

Abstract

Accelerator-based intense epithermal neutron sources for Neutron Capture Therapy (NCT) have been considered as an alternative to nuclear reactors. Lithium (Li) has generally received the widest attention for this application, since the threshold energy is low and neutron yield is high. Because of the poor thermal and chemical properties of Li and the need for heat removal in the target, the design of Li targets has been quite difficult. Beryllium (Be) has been thought of as an alternative target because of its good thermal and chemical properties and reasonable neutron yield. However, in order to have a neutron yield comparable to that of a thick Li target bombarded with 2.5 MeV protons, the proton energy required for a thick Be target must be approaching 4 MeV. Consequently, the neutrons emitted are more energetic. In addition, a significant amount of high-energy gamma rays, which is undesirable, will occur when Be is bombarded with low-energy protons. Regardless of the more energetic neutrons and additional gamma rays, in this paper it is shown that it is possible to develop a high-quality and high-intensity epithermal neutron beam based on a thick Be target for NCT treatment. For a fixed proton current, the optimal Be-target-based beam (with 4-MeV protons) can produce a neutron beam, with both quality and intensity slightly better than those produced by the optimal Li-target-based beam (with 2.5-MeV protons). The single-session NCT treatment time for the optimal Be-target-based beam is estimated to be 88 min for a proton current of 50 mA.(ABSTRACT TRUNCATED AT 250 WORDS)

摘要

用于中子俘获疗法(NCT)的基于加速器的强超热中子源已被视为核反应堆的替代方案。锂(Li)在该应用中通常受到最广泛关注,因为其阈能低且中子产额高。由于锂的热学和化学性质较差以及靶体需要散热,锂靶的设计颇具难度。铍(Be)因其良好的热学和化学性质以及合理的中子产额而被视为替代靶材。然而,为了使厚铍靶的中子产额与被2.5兆电子伏特质子轰击的厚锂靶相当,厚铍靶所需的质子能量必须接近4兆电子伏特。因此,发射出的中子能量更高。此外,用低能质子轰击铍时会产生大量 undesirable 的高能伽马射线。尽管存在能量更高的中子和额外的伽马射线,但本文表明,基于厚铍靶开发用于NCT治疗的高质量、高强度超热中子束是可行的。对于固定的质子电流,基于铍靶的最佳束流(用4兆电子伏特质子)产生的中子束,其质量和强度略优于基于锂靶的最佳束流(用2.5兆电子伏特质子)。对于50毫安的质子电流,基于铍靶的最佳束流单次NCT治疗时间估计为88分钟。(摘要截断于250字)

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