{"title":"一些中子在1478兆电子伏时的活化截面","authors":"J.C. Robertson , B. Audric, P. Kolkowski","doi":"10.1016/0022-3107(73)90084-1","DOIUrl":null,"url":null,"abstract":"<div><p>Fast neutron activation cross-sections have been measured at 14·78 MeV relative to the <sup>56</sup>Fe(<em>n,p</em>)<sup>56</sup>Mn cross-section. The following cross-sections (in millibarns) have been determined: <sup>14</sup>N(<em>n, 2n</em>)<sup>13</sup>N 7·45 ± 0·4, <sup>19</sup>F(<em>n, 2n</em>)<sup>18</sup>F 47·9 ± 1·4, <sup>65</sup>Cu(<em>n, 2n</em>)<sup>64</sup>Cu 1043 ± 37·7, <sup>160</sup>Gd(<em>n, 2n</em>)<sup>159</sup>Gd 1456 ± 44, <sup>198</sup>Pt(<em>n, 2n</em>)<sup>197</sup>Pt 2091 ±113, <sup>27</sup>Al(<em>n</em>, α)<sup>24</sup>Na 115·5 ± 3, <sup>30</sup>Si(<em>n</em>, α)<sup>30</sup>Mg 90 ± 11, <sup>34</sup>S(<em>n</em>, α) <sup>31</sup>Si 194 ± 5·9, <sup>51</sup>V(<em>n</em>, α)<sup>48</sup>Sc 19·5 ± 1·2, <sup>59</sup>Co(<em>n, α</em>)<sup>56</sup>Mn 32·3 ± 1·1, <sup>24</sup>Mg(<em>n,p</em>)<sup>24</sup>Na 179·7 ± 5, <sup>27</sup>Al(<em>n,p</em>)<sup>27</sup>Mg 68 ± 2·3, <sup>28</sup>Si(<em>n,p</em>)<sup>28</sup>Al 265 ± 7·5, <sup>29</sup>Si(<em>n,p</em>)<sup>29</sup>Al 131 ± 13·6, <sup>31</sup>P(<em>n,p</em>)<sup>31</sup>Si 85·6 ± 2·6 <sup>32</sup>S(<em>n, p</em>)<sup>32</sup>P 219 ± 7·1, <sup>51</sup>V(<em>n,p</em>)<sup>51</sup>Ti 31 ± 1·3, <sup>65</sup>Cu(<em>n,p</em>)<sup>65</sup>Ni 26 ± 1. The samples were in the form of thin foils and the activities produced after irradiation were determined using absolute 4πβ-γ coincidence counting techniques. The Value of the <sup>56</sup>Fe(<em>n, p</em>)<sup>56</sup>Mn cross-section used as the standard was 109·8 ± 2·9 mb. The results are compared with those of other authors and show that by considering the ratio of individual cross-sections it is possible to determine if a single cross-section is grossly in error or not.</p></div>","PeriodicalId":100811,"journal":{"name":"Journal of Nuclear Energy","volume":"27 8","pages":"Pages 531-541"},"PeriodicalIF":0.0000,"publicationDate":"1973-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-3107(73)90084-1","citationCount":"30","resultStr":"{\"title\":\"Some neutron activation cross-sections at 1478 MeV\",\"authors\":\"J.C. Robertson , B. Audric, P. Kolkowski\",\"doi\":\"10.1016/0022-3107(73)90084-1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Fast neutron activation cross-sections have been measured at 14·78 MeV relative to the <sup>56</sup>Fe(<em>n,p</em>)<sup>56</sup>Mn cross-section. The following cross-sections (in millibarns) have been determined: <sup>14</sup>N(<em>n, 2n</em>)<sup>13</sup>N 7·45 ± 0·4, <sup>19</sup>F(<em>n, 2n</em>)<sup>18</sup>F 47·9 ± 1·4, <sup>65</sup>Cu(<em>n, 2n</em>)<sup>64</sup>Cu 1043 ± 37·7, <sup>160</sup>Gd(<em>n, 2n</em>)<sup>159</sup>Gd 1456 ± 44, <sup>198</sup>Pt(<em>n, 2n</em>)<sup>197</sup>Pt 2091 ±113, <sup>27</sup>Al(<em>n</em>, α)<sup>24</sup>Na 115·5 ± 3, <sup>30</sup>Si(<em>n</em>, α)<sup>30</sup>Mg 90 ± 11, <sup>34</sup>S(<em>n</em>, α) <sup>31</sup>Si 194 ± 5·9, <sup>51</sup>V(<em>n</em>, α)<sup>48</sup>Sc 19·5 ± 1·2, <sup>59</sup>Co(<em>n, α</em>)<sup>56</sup>Mn 32·3 ± 1·1, <sup>24</sup>Mg(<em>n,p</em>)<sup>24</sup>Na 179·7 ± 5, <sup>27</sup>Al(<em>n,p</em>)<sup>27</sup>Mg 68 ± 2·3, <sup>28</sup>Si(<em>n,p</em>)<sup>28</sup>Al 265 ± 7·5, <sup>29</sup>Si(<em>n,p</em>)<sup>29</sup>Al 131 ± 13·6, <sup>31</sup>P(<em>n,p</em>)<sup>31</sup>Si 85·6 ± 2·6 <sup>32</sup>S(<em>n, p</em>)<sup>32</sup>P 219 ± 7·1, <sup>51</sup>V(<em>n,p</em>)<sup>51</sup>Ti 31 ± 1·3, <sup>65</sup>Cu(<em>n,p</em>)<sup>65</sup>Ni 26 ± 1. The samples were in the form of thin foils and the activities produced after irradiation were determined using absolute 4πβ-γ coincidence counting techniques. The Value of the <sup>56</sup>Fe(<em>n, p</em>)<sup>56</sup>Mn cross-section used as the standard was 109·8 ± 2·9 mb. The results are compared with those of other authors and show that by considering the ratio of individual cross-sections it is possible to determine if a single cross-section is grossly in error or not.</p></div>\",\"PeriodicalId\":100811,\"journal\":{\"name\":\"Journal of Nuclear Energy\",\"volume\":\"27 8\",\"pages\":\"Pages 531-541\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1973-08-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0022-3107(73)90084-1\",\"citationCount\":\"30\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Nuclear Energy\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0022310773900841\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Nuclear Energy","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0022310773900841","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 30
摘要
在相对于56Fe(n,p)56Mn截面的14.78 MeV下测量了快中子激活截面。以下横截面(以毫巴计)已被确定:14 n (2 n) 13 n 7·45±0·4,19 f (n, 2 n) 18 f 47 * 9±1 * 4,65立方(2 n) 64铜1043±37·7、160 gd (2 n) 159 gd 1456±44岁198 pt (2 n) 197 pt 2091±113、27 al (n,α)24 na 115·5±3,30 si (n,α)30毫克90±11日34 s (n,α)31 si 194±5·9日51 v (n,α)48 sc 19 * 5±1 * 2,59有限公司(n,α)56 mn 32 * 3±1 * 1,24毫克(n, p) 24 na 179·7±5,27(氮、磷)27毫克68±2·3、28 si(氮、磷)28 al 265±7·5,29 si (n, p) 29 al 131±13·31 p (n, p) 31 si 85·6±2·6 32 s (n, p) 32 p 219±7·51 v (n, p) 51 ti 31±1·3,65立方(氮、磷)65 ni 26±1。样品呈薄片状,辐照后的活度采用绝对4πβ-γ符合计数法测定。作为标准的56Fe(n, p)56Mn截面值为109·8±2·9 mb,并与其他作者的结果进行了比较,结果表明,通过考虑单个截面的比值,可以确定单个截面是否有严重误差。
Some neutron activation cross-sections at 1478 MeV
Fast neutron activation cross-sections have been measured at 14·78 MeV relative to the 56Fe(n,p)56Mn cross-section. The following cross-sections (in millibarns) have been determined: 14N(n, 2n)13N 7·45 ± 0·4, 19F(n, 2n)18F 47·9 ± 1·4, 65Cu(n, 2n)64Cu 1043 ± 37·7, 160Gd(n, 2n)159Gd 1456 ± 44, 198Pt(n, 2n)197Pt 2091 ±113, 27Al(n, α)24Na 115·5 ± 3, 30Si(n, α)30Mg 90 ± 11, 34S(n, α) 31Si 194 ± 5·9, 51V(n, α)48Sc 19·5 ± 1·2, 59Co(n, α)56Mn 32·3 ± 1·1, 24Mg(n,p)24Na 179·7 ± 5, 27Al(n,p)27Mg 68 ± 2·3, 28Si(n,p)28Al 265 ± 7·5, 29Si(n,p)29Al 131 ± 13·6, 31P(n,p)31Si 85·6 ± 2·6 32S(n, p)32P 219 ± 7·1, 51V(n,p)51Ti 31 ± 1·3, 65Cu(n,p)65Ni 26 ± 1. The samples were in the form of thin foils and the activities produced after irradiation were determined using absolute 4πβ-γ coincidence counting techniques. The Value of the 56Fe(n, p)56Mn cross-section used as the standard was 109·8 ± 2·9 mb. The results are compared with those of other authors and show that by considering the ratio of individual cross-sections it is possible to determine if a single cross-section is grossly in error or not.