10B(p, αγ1)7Be, 10B(p, p'γ1)10B 和 11B(p, p'γ1) 11B 反应的差分截面测量结果

IF 1.4 3区 物理与天体物理 Q3 INSTRUMENTS & INSTRUMENTATION
Hafez Taghipour Aslani , Alireza Jokar , Ali Akbar Mehmandoost-Khajeh-Dad , Hossien Rafi-Kheiri
{"title":"10B(p, αγ1)7Be, 10B(p, p'γ1)10B 和 11B(p, p'γ1) 11B 反应的差分截面测量结果","authors":"Hafez Taghipour Aslani ,&nbsp;Alireza Jokar ,&nbsp;Ali Akbar Mehmandoost-Khajeh-Dad ,&nbsp;Hossien Rafi-Kheiri","doi":"10.1016/j.nimb.2024.165509","DOIUrl":null,"url":null,"abstract":"<div><p>Differential cross-sections of the <sup>10</sup>B(p, αγ<sub>1</sub>)<sup>7</sup>Be (E<sub>γ</sub> = 429 keV), <sup>10</sup>B(p, p’γ<sub>1</sub>)<sup>10</sup>B (E<sub>γ</sub> = 718 keV) and <sup>11</sup>B(p, p’γ<sub>1</sub>) <sup>11</sup>B (E<sub>γ</sub> = 2124 keV) reactions have been measured at proton laboratory energies of 912–2776 keV at 90<sup>°</sup>. The proton beam impinged on a thin <sup>nat</sup>B<sub>2</sub>O<sub>3</sub> film evaporated onto a self-supporting thin carbon layer. The incident energies were increased by 10 (20) keV steps in the resonance (off-resonance) regions. Our data are compared with the existing ones from literature. A benchmark procedure was performed by comparing the calculated thick-target yields from the current differential cross-sections with the existing measured thick target gamma-ray yields. The overall systematic uncertainty of the cross-sections was estimated to be about 10 %, mainly related to the target thickness determination.</p></div>","PeriodicalId":19380,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","volume":"556 ","pages":"Article 165509"},"PeriodicalIF":1.4000,"publicationDate":"2024-08-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Differential cross-section measurement for 10B(p, αγ1)7Be, 10B(p, p’γ1)10B and 11B(p, p’γ1) 11B reactions\",\"authors\":\"Hafez Taghipour Aslani ,&nbsp;Alireza Jokar ,&nbsp;Ali Akbar Mehmandoost-Khajeh-Dad ,&nbsp;Hossien Rafi-Kheiri\",\"doi\":\"10.1016/j.nimb.2024.165509\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Differential cross-sections of the <sup>10</sup>B(p, αγ<sub>1</sub>)<sup>7</sup>Be (E<sub>γ</sub> = 429 keV), <sup>10</sup>B(p, p’γ<sub>1</sub>)<sup>10</sup>B (E<sub>γ</sub> = 718 keV) and <sup>11</sup>B(p, p’γ<sub>1</sub>) <sup>11</sup>B (E<sub>γ</sub> = 2124 keV) reactions have been measured at proton laboratory energies of 912–2776 keV at 90<sup>°</sup>. The proton beam impinged on a thin <sup>nat</sup>B<sub>2</sub>O<sub>3</sub> film evaporated onto a self-supporting thin carbon layer. The incident energies were increased by 10 (20) keV steps in the resonance (off-resonance) regions. Our data are compared with the existing ones from literature. A benchmark procedure was performed by comparing the calculated thick-target yields from the current differential cross-sections with the existing measured thick target gamma-ray yields. The overall systematic uncertainty of the cross-sections was estimated to be about 10 %, mainly related to the target thickness determination.</p></div>\",\"PeriodicalId\":19380,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"volume\":\"556 \",\"pages\":\"Article 165509\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2024-08-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168583X24002799\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"INSTRUMENTS & INSTRUMENTATION\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168583X24002799","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
引用次数: 0

摘要

在质子实验室能量为 912-2776 keV、90° 时,测量了 10Be(p,αγ1)7Be(Eγ = 429 keV)、10Be(p,p'γ1)10B(Eγ = 718 keV)和 11Be(p,p'γ1)11B(Eγ = 2124 keV)反应的差分截面。质子束撞击在蒸发到自支撑薄碳层上的 natB2O3 薄膜上。在共振(非共振)区域,入射能量以 10 (20) keV 为单位递增。我们的数据与现有的文献数据进行了比较。通过比较当前差分截面计算出的厚靶伽马射线产率和现有测量的厚靶伽马射线产率,执行了一个基准程序。据估计,截面的总体系统不确定性约为 10%,主要与目标厚度的确定有关。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Differential cross-section measurement for 10B(p, αγ1)7Be, 10B(p, p’γ1)10B and 11B(p, p’γ1) 11B reactions

Differential cross-sections of the 10B(p, αγ1)7Be (Eγ = 429 keV), 10B(p, p’γ1)10B (Eγ = 718 keV) and 11B(p, p’γ1) 11B (Eγ = 2124 keV) reactions have been measured at proton laboratory energies of 912–2776 keV at 90°. The proton beam impinged on a thin natB2O3 film evaporated onto a self-supporting thin carbon layer. The incident energies were increased by 10 (20) keV steps in the resonance (off-resonance) regions. Our data are compared with the existing ones from literature. A benchmark procedure was performed by comparing the calculated thick-target yields from the current differential cross-sections with the existing measured thick target gamma-ray yields. The overall systematic uncertainty of the cross-sections was estimated to be about 10 %, mainly related to the target thickness determination.

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
CiteScore
2.80
自引率
7.70%
发文量
231
审稿时长
1.9 months
期刊介绍: Section B of Nuclear Instruments and Methods in Physics Research covers all aspects of the interaction of energetic beams with atoms, molecules and aggregate forms of matter. This includes ion beam analysis and ion beam modification of materials as well as basic data of importance for these studies. Topics of general interest include: atomic collisions in solids, particle channelling, all aspects of collision cascades, the modification of materials by energetic beams, ion implantation, irradiation - induced changes in materials, the physics and chemistry of beam interactions and the analysis of materials by all forms of energetic radiation. Modification by ion, laser and electron beams for the study of electronic materials, metals, ceramics, insulators, polymers and other important and new materials systems are included. Related studies, such as the application of ion beam analysis to biological, archaeological and geological samples as well as applications to solve problems in planetary science are also welcome. Energetic beams of interest include atomic and molecular ions, neutrons, positrons and muons, plasmas directed at surfaces, electron and photon beams, including laser treated surfaces and studies of solids by photon radiation from rotating anodes, synchrotrons, etc. In addition, the interaction between various forms of radiation and radiation-induced deposition processes are relevant.
×
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