Secondary nuclear reactions induced in tin by fast protons

M.Ia. Kuznetsova, V.N. Mekhedov, V.A. Khalkin
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Abstract

Nuclear reactions in which spallation products are captured by the target nucleus have been studied by the radio-chemical method. The excitation functions of secondary reactions leading to product nuclei having charges 2 or 3 units greater than that of the target nuclei have been obtained from measurements of the yields of isotopes of tellurium (Z = 52) and iodine (Z = 53) formed in the 170–660 MeV proton bombardment of tin (Z = 50). The cross-sections of these reactions increase with increasing proton energy: for Ep = 170 MeV, σ(α, xn) and σ(Li, xn) are 18·5 ± 5 and 0·17 ± 0·1 μbarns, respectively; for Ep = 660 MeV, these cross-sections are 50 ± 6·5 and 1·6 ± 0·5 μbarns, respectively. The cross-sections for the capture of lithium nuclei by tin obtained in this work are in good agreement with the results for similar reactions with copper, tin, and lead over a comparable proton energy interval but they are 50 times less than the cross-sections found by Marquez and Perlman. The observed secondary reaction cross-sections for the capture of lithium nuclei can be accounted for only by supposing that the lithium nuclei are emitted with energies greater than they could acquire as a result of fission or evaporation of the target nucleus. Secondary reactions of the type (α, xn) can be accounted for by assuming that the m-particles are emitted as a result of the evaporation process.

快质子在锡中引起的二次核反应
用放射化学方法研究了靶核捕获散裂产物的核反应。对170-660 MeV质子轰击锡(Z = 50)形成的碲(Z = 52)和碘(Z = 53)同位素的产率进行了测量,得到了导致产物原子核的电荷比靶核大2或3个单位的二次反应的激发函数。这些反应的横截面随着质子能量的增加而增大:Ep = 170 MeV时,σ(α, xn)和σ(Li, xn)分别为18.5±5和0.17±0.1 μbarns;当Ep = 660 MeV时,这些截面分别为50±6.5 μbarn和1.6±0.5 μbarn。在这项工作中获得的锡捕获锂核的截面与铜、锡和铅在类似质子能量区间内的类似反应的结果非常一致,但它们比Marquez和Perlman发现的截面小50倍。所观察到的捕获锂核的二次反应截面只能通过假设锂核发射的能量大于它们作为目标核裂变或蒸发的结果所能获得的能量来解释。(α, xn)类型的二次反应可以通过假设m粒子是由于蒸发过程而发射来解释。
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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