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在日本理化研究所利用7Li(p,n)7Be反应在250至390 MeV能量范围内开发准单能中子场。

Development of a quasi-monoenergetic neutron field using the 7Li(p,n)7Be reaction in the energy range from 250 to 390 MeV at RCNP.

作者信息

Taniguchi S, Nakao N, Nakamura T, Yashima H, Iwamoto Y, Satoh D, Nakane Y, Nakashima H, Itoga T, Tamii A, Hatanaka K

机构信息

Japan Synchrotron Radiation Research Institute, 1-1-1, Kouto, Mikazuki-cho, Sayo-gun, Hyogo 679-5198, Japan.

出版信息

Radiat Prot Dosimetry. 2007;126(1-4):23-7. doi: 10.1093/rpd/ncm007. Epub 2007 May 13.

Abstract

A quasi-monoenergetic neutron field using the (7)Li(p,n)(7)Be reaction has been developed at the ring cyclotron facility at the Research Center for Nuclear Physics (RCNP), Osaka University. Neutrons were generated from a 10-mm-thick Li target injected by 250, 350 and 392 MeV protons and neutrons produced at 0 degrees were extracted into the time-of-flight (TOF) room of 100-m length through the concrete collimator of 10 x 12 cm aperture and 150 cm thickness. The neutron energy spectra were measured by a 12.7-cm diam x 12.7-cm long NE213 organic liquid scintillator using the TOF method. The peak neutron fluence was 1.94 x 10(10), 1.07 x 10(10) and 1.50 x 10(10) n sr(-1) per muC of 250, 350 and 392 MeV protons, respectively. The neutron spectra generated from various thick (stopping length) targets of carbon, aluminium, iron and lead, bombarded by 250 and 350 MeV protons, were also measured with the TOF method. Although these measurements were performed to obtain thick target neutron yields, they are also used as a continuous energy neutron field. These neutron fields are very useful for characterising neutron detectors, measuring neutron cross sections, testing irradiation effects for various materials and performing neutron shielding experiments.

摘要

大阪大学核物理研究中心的环形回旋加速器设施已开发出一种利用(7)Li(p,n)(7)Be反应的准单能中子场。中子由厚度为10毫米的锂靶产生,该靶由250、350和392兆电子伏的质子注入,在0度产生的中子通过孔径为10×12厘米、厚度为150厘米的混凝土准直器被提取到长度为100米的飞行时间(TOF)室。中子能谱通过一个直径为12.7厘米、长为12.7厘米的NE213有机液体闪烁体,采用飞行时间法进行测量。每微库250、350和392兆电子伏质子的峰值中子注量分别为1.94×10(10)、1.07×10(10)和1.50×10(10)n sr(-1)……(注:原文此处“每微库250、350和392兆电子伏质子的峰值中子注量分别为1.94×10(10)、1.07×10(10)和1.50×10(10)n sr(-1)”后面似乎表述不完整)还采用飞行时间法测量了由250和350兆电子伏质子轰击的碳、铝、铁和铅等各种厚(阻止长度)靶产生的中子谱。尽管进行这些测量是为了获得厚靶中子产额,但它们也被用作连续能量中子场。这些中子场对于表征中子探测器、测量中子截面、测试各种材料的辐照效应以及进行中子屏蔽实验非常有用。 (注:原文中部分括号内容可能表述有误或不完整,翻译时尽量按原文呈现)

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