Determination of the Secondary Neutron Flux at the Massive Natural Uranium Spallation Target

M. Zeman , J. Adam , A.A. Baldin , W.I. Furman , S.A. Gustov , K. Katovsky , J. Khushvaktov , I.I. Mar‘in , F. Novotny , A.A. Solnyshkin , P. Tichy , V.M. Tsoupko-Sitnikov , S.I. Tyutyunnikov , R. Vespalec , J. Vrzalova , V. Wagner , L. Zavorka
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Abstract

The flux of secondary neutrons generated in collisions of the 660 MeV proton beam with the massive natural uranium spallation target was investigated using a set of monoisotopic threshold activation detectors. Sandwiches made of thin high-purity Al, Co, Au, and Bi metal foils were installed in different positions across the whole spallation target. The gamma-ray activity of products of (n,xn) and other studied reactions was measured offline with germanium semiconductor detectors. Reaction yields of radionuclides with half-life exceeding 100 min and with effective neutron energy thresholds between 3.6 MeV and 186 MeV provided us with information about the spectrum of spallation neutrons in this energy region and beyond. The experimental neutron flux was determined using the measured reaction yields and cross-sections calculated with the TALYS 1.8 nuclear reaction program and INCL4-ABLA event generator of MCNP6. Neutron spectra in the region of activation sandwiches were also modeled with the radiation transport code MCNPX 2.7. Neutron flux based on excitation functions from TALYS provides a reasonable description of the neutron spectrum inside the spallation target and is in good agreement with Monte-Carlo predictions. The experimental flux that uses INCL4 cross-sections rather underestimates the modeled spectrum in the whole region of interest, but the agreement within few standard deviations was reached as well. The paper summarizes basic principles of the method for determining the spectrum of high-energy neutrons without employing the spectral adjustment routines and points out to the need for model improvements and precise cross-section measurements.

天然铀散裂靶处二次中子通量的测定
利用单同位素阈值激活探测器,研究了660mev质子束与大质量天然铀散裂靶碰撞时产生的次级中子通量。由高纯度的薄铝、钴、金和铋金属箔制成的三明治被安装在整个散裂靶的不同位置。(n,xn)和其他研究反应产物的伽马射线活度用锗半导体探测器离线测量。半衰期超过100 min、有效中子能量阈值在3.6 MeV ~ 186 MeV之间的放射性核素的反应产额为我们提供了该能量区及以上的散裂中子谱信息。实验中子通量的测定采用了TALYS 1.8核反应程序和MCNP6的INCL4-ABLA事件发生器计算的反应产率和截面。利用辐射输运程序MCNPX 2.7对活化夹层区的中子能谱进行了模拟。基于TALYS激发函数的中子通量对散裂靶内的中子谱进行了合理的描述,与蒙特卡罗预测结果吻合较好。使用INCL4截面的实验通量大大低估了整个感兴趣区域的模拟光谱,但在几个标准差范围内也达到了一致。本文总结了不采用谱平差方法测定高能中子谱的基本原理,指出了改进模型和精确测量截面的必要性。
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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