Measurement of Cross Sections of Reactions \({}^{191}\)Ir(\({{p},{pxn}}\))\({}^{189,190}\)Ir,\({}^{193}\)Ir(\({{p},{pn}}\))\({}^{192}\)Ir, and \({}^{191}\)Ir(\({{p},{xn}}\))\({}^{188,189}\)Pt and Cumulative Cross Sections of Reactions \({}^{191}\)Ir(\({{p},{n}}\))\({}^{191}\textrm{Pt}+{}^{193}\)Ir(\({{p},3{n}}\))\({}^{191}\)Pt during Irradiation of Natural Iridium Target with \({}^{1}\)H Nuclei

IF 0.5 4区 物理与天体物理 Q4 PHYSICS, NUCLEAR
T. M. Fazliev, R. A. Aliev, V. A. Zagryadskiy, E. S. Kormazeva, T. M. Kuznetsova, T. Yu. Malamut, V. I. Novikov, I. N. Popov
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引用次数: 0

Abstract

This article addresses measurement of the cross sections of the reactions \({}^{191}\)Ir(\(p,pn\))\({}^{190}\)Ir, \({}^{193}\)Ir(\(p,pn\))\({}^{192}\)Ir, \({}^{191}\)Ir(\(p,4n\))\({}^{188}\)Pt, \({}^{191}\)Ir(\(p,3n\))\({}^{189}\)Pt, and \({}^{191}\)Ir(\(p,p2n\))\({}^{189}\)Ir and the cumulative cross section of the reaction \({}^{193}\)Ir(\(p,3n\))\({}^{191}\textrm{Pt}+{}^{191}\)Ir(\(p,n\))\({}^{191}\)Pt in the proton energy range of 29.6–17.2 MeV during proton irradiation of a target of natural metal iridium on the U-150 cyclotron of the National Research Center (NRC) Kurchatov Institute. The experimental cross sections of the reactions were compared with data of TENDL-2023. The results of this study make it possible to evaluate the effectiveness of the production of the target radioisotope \({}^{189}\)Ir, a precursor in a \({}^{189}\textrm{Ir}/{}^{189m}\)Os isotope generator of an Auger emitter and conversion electrons from \({}^{189m}\)Os, which can be used as a low-dose therapeutic agent in nuclear medicine. Experimental cross sections of the formation of accompanying radionuclide impurities enable development of an optimal radiochemical technique for release of the radioisotope \({}^{189}\)Ir from a proton-irradiated iridium target.

Abstract Image

反应截面的测量 \({}^{191}\)Ir(\({{p},{pxn}}\))\({}^{189,190}\)嗯,\({}^{193}\)Ir(\({{p},{pn}}\))\({}^{192}\)Ir, and \({}^{191}\)Ir(\({{p},{xn}}\))\({}^{188,189}\)Pt和反应的累积截面 \({}^{191}\)Ir(\({{p},{n}}\))\({}^{191}\textrm{Pt}+{}^{193}\)Ir(\({{p},3{n}}\))\({}^{191}\)天然铱靶辐照过程中的铂 \({}^{1}\)氢原子核
本文讨论了反应截面的测量 \({}^{191}\)Ir(\(p,pn\))\({}^{190}\)嗯, \({}^{193}\)Ir(\(p,pn\))\({}^{192}\)嗯, \({}^{191}\)Ir(\(p,4n\))\({}^{188}\)Pt, \({}^{191}\)Ir(\(p,3n\))\({}^{189}\)Pt, and \({}^{191}\)Ir(\(p,p2n\))\({}^{189}\)Ir和反应的累积截面 \({}^{193}\)Ir(\(p,3n\))\({}^{191}\textrm{Pt}+{}^{191}\)Ir(\(p,n\))\({}^{191}\)库尔恰托夫国家研究中心(NRC)库尔恰托夫研究所U-150回旋加速器质子辐照天然金属铱靶时,质子能量范围为29.6-17.2 MeV的铂。实验反应截面与TENDL-2023的数据进行了比较。这项研究的结果使评估目标放射性同位素生产的有效性成为可能 \({}^{189}\)Ir, a的前体 \({}^{189}\textrm{Ir}/{}^{189m}\)俄歇发射器和转换电子的Os同位素发生器 \({}^{189m}\)可作为核医学的低剂量治疗剂。伴随放射性核素杂质形成的实验横截面有助于开发释放放射性同位素的最佳放射化学技术 \({}^{189}\)来自质子辐照的铱靶。
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来源期刊
Physics of Atomic Nuclei
Physics of Atomic Nuclei 物理-物理:核物理
CiteScore
0.60
自引率
25.00%
发文量
56
审稿时长
3-6 weeks
期刊介绍: Physics of Atomic Nuclei is a journal that covers experimental and theoretical studies of nuclear physics: nuclear structure, spectra, and properties; radiation, fission, and nuclear reactions induced by photons, leptons, hadrons, and nuclei; fundamental interactions and symmetries; hadrons (with light, strange, charm, and bottom quarks); particle collisions at high and superhigh energies; gauge and unified quantum field theories, quark models, supersymmetry and supergravity, astrophysics and cosmology.
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