{"title":"14N +175Lu体系聚变-裂变截面的综合活化分析","authors":"Satyendra Kumar Gautam , Manoj Kumar Sharma , Sushant Arora , Mamta Sarswat , Aquib Siddique , M. Shariq Asnain , Mohd. Shuaib , Ishfaq Majeed , Abhishek Yadav , Puspendra P. Singh , B.P. Singh , R. Prasad","doi":"10.1016/j.nuclphysa.2026.123341","DOIUrl":null,"url":null,"abstract":"<div><div>The experiments for measuring the cross sections of 35 fission-like residues (with mass numbers 74 ≤ A ≤ 111) and 10 fusion-like residues have been carried out at energies ≈ 72.7 MeV, 80.3 MeV and 88.0 MeV. In this measurement, the recoil catcher technique followed by an off-beam activation <em>γ</em>-ray spectroscopy is used. The analysis of fusion cross-section data with code PACE4 reveals the contribution of complete and incomplete fusion processes in <sup>14</sup>N +<sup>175</sup>Lu reactions. Fission fragments produced as a result of fusion of <sup>14</sup>N projectile with <sup>175</sup>Lu target have also been confirmed by comparing the values of post-fission observables viz., mass (<em>σ<sub>A</sub></em>) and charge (<em>σ<sub>Z</sub></em>) dispersions (deduced from the isotopic mass and isobaric yield distributions) with literature data. In addition to this, the statistical scission-point model based theoretical calculations performed (as per the prescription of Gubbi et. al., [31]) for determining the charge dispersion (<em>σ<sub>Z</sub></em>) of Br and Kr isotopes validate the experimental values of <em>σ<sub>Z</sub></em> obtained from the isobaric yield distribution. Thus, the consistency between theoretical and experimental values of charge dispersion (<em>σ<sub>Z</sub></em>) indicates the production of fission fragments from a equilibrated compound nucleus <sup>189</sup><em>Pt</em>* in <sup>14</sup>N +<sup>175</sup>Lu reactions. In the present work, an alternative method is used for converting isotopic mass distribution into isobaric yield distribution. Furthermore, the experimental finding of mass variance (<span><math><msubsup><mi>σ</mi><mi>M</mi><mn>2</mn></msubsup></math></span>) of fission fragments also complements the investigations of mass (<em>σ<sub>A</sub></em>) and charge (<em>σ<sub>Z</sub></em>) dispersions, as width of mass distribution (i.e., mass variance, <span><math><msubsup><mi>σ</mi><mi>M</mi><mn>2</mn></msubsup></math></span>) of fission fragments is found to be exponentially function of excitation energy, hence, temperature of equilibrated compound nucleus.</div></div>","PeriodicalId":19246,"journal":{"name":"Nuclear Physics A","volume":"1068 ","pages":"Article 123341"},"PeriodicalIF":1.9000,"publicationDate":"2026-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A comprehensive activation analysis of fusion-fission cross-sections for 14N +175Lu system\",\"authors\":\"Satyendra Kumar Gautam , Manoj Kumar Sharma , Sushant Arora , Mamta Sarswat , Aquib Siddique , M. 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Fission fragments produced as a result of fusion of <sup>14</sup>N projectile with <sup>175</sup>Lu target have also been confirmed by comparing the values of post-fission observables viz., mass (<em>σ<sub>A</sub></em>) and charge (<em>σ<sub>Z</sub></em>) dispersions (deduced from the isotopic mass and isobaric yield distributions) with literature data. In addition to this, the statistical scission-point model based theoretical calculations performed (as per the prescription of Gubbi et. al., [31]) for determining the charge dispersion (<em>σ<sub>Z</sub></em>) of Br and Kr isotopes validate the experimental values of <em>σ<sub>Z</sub></em> obtained from the isobaric yield distribution. Thus, the consistency between theoretical and experimental values of charge dispersion (<em>σ<sub>Z</sub></em>) indicates the production of fission fragments from a equilibrated compound nucleus <sup>189</sup><em>Pt</em>* in <sup>14</sup>N +<sup>175</sup>Lu reactions. In the present work, an alternative method is used for converting isotopic mass distribution into isobaric yield distribution. Furthermore, the experimental finding of mass variance (<span><math><msubsup><mi>σ</mi><mi>M</mi><mn>2</mn></msubsup></math></span>) of fission fragments also complements the investigations of mass (<em>σ<sub>A</sub></em>) and charge (<em>σ<sub>Z</sub></em>) dispersions, as width of mass distribution (i.e., mass variance, <span><math><msubsup><mi>σ</mi><mi>M</mi><mn>2</mn></msubsup></math></span>) of fission fragments is found to be exponentially function of excitation energy, hence, temperature of equilibrated compound nucleus.</div></div>\",\"PeriodicalId\":19246,\"journal\":{\"name\":\"Nuclear Physics A\",\"volume\":\"1068 \",\"pages\":\"Article 123341\"},\"PeriodicalIF\":1.9000,\"publicationDate\":\"2026-04-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Physics A\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0375947426000199\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2026/1/24 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Physics A","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0375947426000199","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2026/1/24 0:00:00","PubModel":"Epub","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
引用次数: 0
摘要
实验测量了35个质量数为74 ≤ A ≤ 111的类裂变残基和10个能量为 ≈ 72.7 MeV、80.3 MeV和88.0 MeV的类聚变残基的截面。在这个测量中,后坐力捕捉技术随后的离束激活γ射线光谱被使用。用PACE4代码对核聚变截面数据进行分析,揭示了完全核聚变和不完全核聚变对14N +175Lu反应的贡献。通过将裂变后的质量(σA)和电荷(σZ)色散值(由同位素质量和等压产率分布推导而来)与文献数据进行比较,证实了14N弹丸与175Lu靶融合产生的裂变碎片。此外,基于统计断裂点模型的理论计算(按照Gubbi et al.,[31]的规定)确定了Br和Kr同位素的电荷色散(σZ),验证了从等压产率分布中得到的σZ的实验值。因此,电荷色散(σZ)的理论值与实验值的一致性表明,在14N +175Lu反应中,平衡复合核189Pt*产生了裂变碎片。在本工作中,采用了另一种方法将同位素质量分布转化为等压产率分布。此外,裂变碎片的质量方差(σM2)的实验发现也补充了质量(σA)和电荷(σZ)色散的研究,发现裂变碎片的质量分布宽度(即质量方差,σM2)是激发能的指数函数,因此,平衡复合核的温度。
A comprehensive activation analysis of fusion-fission cross-sections for 14N +175Lu system
The experiments for measuring the cross sections of 35 fission-like residues (with mass numbers 74 ≤ A ≤ 111) and 10 fusion-like residues have been carried out at energies ≈ 72.7 MeV, 80.3 MeV and 88.0 MeV. In this measurement, the recoil catcher technique followed by an off-beam activation γ-ray spectroscopy is used. The analysis of fusion cross-section data with code PACE4 reveals the contribution of complete and incomplete fusion processes in 14N +175Lu reactions. Fission fragments produced as a result of fusion of 14N projectile with 175Lu target have also been confirmed by comparing the values of post-fission observables viz., mass (σA) and charge (σZ) dispersions (deduced from the isotopic mass and isobaric yield distributions) with literature data. In addition to this, the statistical scission-point model based theoretical calculations performed (as per the prescription of Gubbi et. al., [31]) for determining the charge dispersion (σZ) of Br and Kr isotopes validate the experimental values of σZ obtained from the isobaric yield distribution. Thus, the consistency between theoretical and experimental values of charge dispersion (σZ) indicates the production of fission fragments from a equilibrated compound nucleus 189Pt* in 14N +175Lu reactions. In the present work, an alternative method is used for converting isotopic mass distribution into isobaric yield distribution. Furthermore, the experimental finding of mass variance () of fission fragments also complements the investigations of mass (σA) and charge (σZ) dispersions, as width of mass distribution (i.e., mass variance, ) of fission fragments is found to be exponentially function of excitation energy, hence, temperature of equilibrated compound nucleus.
期刊介绍:
Nuclear Physics A focuses on the domain of nuclear and hadronic physics and includes the following subsections: Nuclear Structure and Dynamics; Intermediate and High Energy Heavy Ion Physics; Hadronic Physics; Electromagnetic and Weak Interactions; Nuclear Astrophysics. The emphasis is on original research papers. A number of carefully selected and reviewed conference proceedings are published as an integral part of the journal.