质子俘获形成表

Rolf Nordhagen
{"title":"质子俘获形成表","authors":"Rolf Nordhagen","doi":"10.1016/0550-306X(67)80008-9","DOIUrl":null,"url":null,"abstract":"<div><p>The values of the parameters for magnetic substate populations and statistical tensors are computed for levels formed by proton capture. The substate population numbers and the tensor parameters are given for levels with spins ranging from <em>J</em> = 1 to <em>J</em> = 6, <em>J</em> integral, and formed by proton capture in channels with spins ranging from <em>s</em> = 0 to <em>s</em> = 4, <em>s</em> integral. The orbital angular momenta range from <em>l</em> = 0 to <em>l</em> = 7.</p><p>The coefficients relating substate populations to tensor parameters are given for spins <em>J</em> = 1 to <em>J</em> = 6, <em>J</em> integral, and for <em>J</em> = 3/2 to 9/2, <em>J</em> half-integral. Extension to <em>J</em> &gt;6 can easily be made with the use of a Clebsch-Gordan subroutine for an electronic computer.</p><p>In most cases half-integral spins are formed by capture in the channel with <em>s</em> = 1/2. The substate populations are then constant, <em>P</em><sub>1/2</sub> = 1. The tensor parameters are then contained in the table of coefficients relating these parameters to the population numbers. The parameters for half-integral spins are not tabulated separately.</p><p>A final table gives the coefficients relating the parameters for the second state excited in the (<em>P,γ</em>) process, to those of the initially formed level, when the primary <em>γ</em>-ray is unobserved but of known multipolarity. Primary spins <em>J</em> = 1 to 6, <em>J</em> integral, and <em>J</em> = 3/2 to 9/2, <em>J</em> half-integral, are entered together with the secondary spins reached by dipole and quadrupole transitions.</p></div>","PeriodicalId":100967,"journal":{"name":"Nuclear Data Sheets. Section A","volume":"3 3","pages":"Pages 363-364"},"PeriodicalIF":0.0000,"publicationDate":"1967-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0550-306X(67)80008-9","citationCount":"2","resultStr":"{\"title\":\"Proton capture formation tables\",\"authors\":\"Rolf Nordhagen\",\"doi\":\"10.1016/0550-306X(67)80008-9\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The values of the parameters for magnetic substate populations and statistical tensors are computed for levels formed by proton capture. The substate population numbers and the tensor parameters are given for levels with spins ranging from <em>J</em> = 1 to <em>J</em> = 6, <em>J</em> integral, and formed by proton capture in channels with spins ranging from <em>s</em> = 0 to <em>s</em> = 4, <em>s</em> integral. The orbital angular momenta range from <em>l</em> = 0 to <em>l</em> = 7.</p><p>The coefficients relating substate populations to tensor parameters are given for spins <em>J</em> = 1 to <em>J</em> = 6, <em>J</em> integral, and for <em>J</em> = 3/2 to 9/2, <em>J</em> half-integral. Extension to <em>J</em> &gt;6 can easily be made with the use of a Clebsch-Gordan subroutine for an electronic computer.</p><p>In most cases half-integral spins are formed by capture in the channel with <em>s</em> = 1/2. The substate populations are then constant, <em>P</em><sub>1/2</sub> = 1. The tensor parameters are then contained in the table of coefficients relating these parameters to the population numbers. The parameters for half-integral spins are not tabulated separately.</p><p>A final table gives the coefficients relating the parameters for the second state excited in the (<em>P,γ</em>) process, to those of the initially formed level, when the primary <em>γ</em>-ray is unobserved but of known multipolarity. Primary spins <em>J</em> = 1 to 6, <em>J</em> integral, and <em>J</em> = 3/2 to 9/2, <em>J</em> half-integral, are entered together with the secondary spins reached by dipole and quadrupole transitions.</p></div>\",\"PeriodicalId\":100967,\"journal\":{\"name\":\"Nuclear Data Sheets. Section A\",\"volume\":\"3 3\",\"pages\":\"Pages 363-364\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1967-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0550-306X(67)80008-9\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Data Sheets. Section A\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0550306X67800089\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Data Sheets. Section A","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0550306X67800089","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2

摘要

对于质子俘获形成的能级,计算了磁基态居群和统计张量的参数值。给出了自旋范围从J = 1到J = 6 (J积分)的能级,以及自旋范围从s = 0到s = 4 (s积分)的通道中质子捕获形成的能级的亚态居族数和张量参数。轨道角动量的范围为l = 0 ~ l = 7。给出了自旋J = 1 ~ J = 6时,子态居群与张量参数的相关系数为J积分,自旋J = 3/2 ~ 9/2时,子态居群与张量参数的半积分。通过使用电子计算机的Clebsch-Gordan子程序可以很容易地对j>6进行扩展。在大多数情况下,半积分自旋是在s = 1/2的通道中捕获形成的。亚态种群是恒定的,P1/2 = 1。张量参数随后包含在这些参数与总体数相关的系数表中。半积分自旋的参数没有单独列出。最后一个表给出了在(P,γ)过程中激发的第二态参数与初始形成水平参数的相关系数,当主γ射线未被观测到但已知多极时。初级自旋J = 1 ~ 6 (J积分)和J = 3/2 ~ 9/2 (J半积分)与偶极子和四极子跃迁达到的次级自旋一起输入。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Proton capture formation tables

The values of the parameters for magnetic substate populations and statistical tensors are computed for levels formed by proton capture. The substate population numbers and the tensor parameters are given for levels with spins ranging from J = 1 to J = 6, J integral, and formed by proton capture in channels with spins ranging from s = 0 to s = 4, s integral. The orbital angular momenta range from l = 0 to l = 7.

The coefficients relating substate populations to tensor parameters are given for spins J = 1 to J = 6, J integral, and for J = 3/2 to 9/2, J half-integral. Extension to J >6 can easily be made with the use of a Clebsch-Gordan subroutine for an electronic computer.

In most cases half-integral spins are formed by capture in the channel with s = 1/2. The substate populations are then constant, P1/2 = 1. The tensor parameters are then contained in the table of coefficients relating these parameters to the population numbers. The parameters for half-integral spins are not tabulated separately.

A final table gives the coefficients relating the parameters for the second state excited in the (P,γ) process, to those of the initially formed level, when the primary γ-ray is unobserved but of known multipolarity. Primary spins J = 1 to 6, J integral, and J = 3/2 to 9/2, J half-integral, are entered together with the secondary spins reached by dipole and quadrupole transitions.

求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信