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靶室结构对中子绝对产额测量的影响

Influence of the target chamber structure on measuring absolute neutron yield
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摘要 介绍了D-T反应使用的结构不同的三种靶室,对不同角度上监测的伴随α粒子谱进行了比较和分析,改进的单管靶室大大地降低了散射的α粒子的本底,α粒子的峰谷比值达到450,α粒子的和峰明显,其计数约占α粒子总数的1.8%,此外,由D(d,p)T反应的能量1.01MeV的氚粒子产生的一个小峰清晰可见。 The three target chambers of different structures adapted in D-T reaction were introduced. Accompanied α-particle spectra at different direction to D+ beam were monitored and compared. Background from scattered α particles was reduced obviously using improved single chamber, and ratio of peak to valley of α-particle spectrum was about 450 : 1. Accounts of sum peak from two α particles were 1.8% of total ones of α-particle spectrum. The small peak of tritium particles with 1.01MeV resulting from D (d, p) T reaction was seen clearly.
作者 陈渊
出处 《核电子学与探测技术》 CAS CSCD 北大核心 2005年第6期584-586,共3页 Nuclear Electronics & Detection Technology
关键词 靶室结构 α粒子谱 中子绝对产额 target chamber structure α-particle spectrum absolute neutron yield
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参考文献2

  • 1Maekawa H, et al. Neutron yield monitors for the fusion neutronics source [R]. JAERI-M report,83-219.
  • 2Novilov VM, et al. Measurement of 14MeV Neutron Multiplication by Total Absorption Method[R]. INDC(eep)-226/G. 1987.

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