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核电厂堆用^(235)U裂变电离室性能影响因素模拟研究 被引量:1
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作者 李群 褚胜男 +2 位作者 黄磊 赵东 夏斌元 《核电子学与探测技术》 CAS 北大核心 2021年第3期443-448,共6页
为了研制性能更加优异的核电厂堆用^(235)U裂变电离室,利用Geant4模拟软件研究了电离室外壳材料、^(235)U镀层厚度、^(235)U丰度及电极间距等参数对电离室性能的影响,并对^(235)U镀层样品进行了拉曼光谱分析。模拟结果表明:(1)1 mm厚的... 为了研制性能更加优异的核电厂堆用^(235)U裂变电离室,利用Geant4模拟软件研究了电离室外壳材料、^(235)U镀层厚度、^(235)U丰度及电极间距等参数对电离室性能的影响,并对^(235)U镀层样品进行了拉曼光谱分析。模拟结果表明:(1)1 mm厚的钛金属可作为堆用裂变电离室外壳;(2)^(235)U镀层最佳厚度约为3μm,镀层厚度的影响机制与“自吸收层”和“出射层”有关;(3)^(235)U丰度变化仅影响电离室探测效率,最佳镀层厚度不变;(4)当可电离气体压强分别为0.1 MPa和0.4 MPa时,电极间距分别大于等于6mm和3mm即可区分U原子衰变产生的a粒子信号。拉曼光谱分析结果表明镀层成分主要为U,O,与所建模型一致,保证了模拟结果的可靠性。 展开更多
关键词 ^^(235)u裂变电离室 GEANT4 ^^(235)u镀层厚度 拉曼光谱
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Calculation of the energy dependence of fission fragments yields and kinetic energy distributions for neutron-induced ^(235)U fission
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作者 Ya-Ning Han Zheng Wei +16 位作者 Yi-Xuan Wang Dong-Ying Huo Peng-Qi Zhang Ming Li Jun Ma Kang Wu Yong-Guang Zheng Yuan He Zhi-Yong Deng Tian-Zhi Jiang Xiang-Lin Zhuo Jin Li Yun Zhang Yu Zhang Jun-Run Wang Xiao-Dong Su Ze-En Yao 《Chinese Physics C》 SCIE CAS CSCD 2024年第8期159-169,共11页
Fission fragments yields and average total kinetic energy are fundamental nuclear data for nuclear energy applications and the study of nuclear devices.Certain fission products,such as ^(95)Zr,^(99)Mo,^(140)Ba,^(144)C... Fission fragments yields and average total kinetic energy are fundamental nuclear data for nuclear energy applications and the study of nuclear devices.Certain fission products,such as ^(95)Zr,^(99)Mo,^(140)Ba,^(144)Ce,and ^(147)Nd,serve as burnup monitors,assessing the number of fissions induced by neutrons on ^(235)U.However,current experimental data for these fission products worldwide are inconsistent,introducing significant uncertainty into related scientific research.In this study,we employed the Potential-driving Model to calculate the independent yields of ^(235)U and evaluate its advantages in such calculations.Additionally,we investigated the energy dependence of independent yields to select important products.Furthermore,we calculated the cumulative yields of ^(95)Zr,^(99)Mo,^(140)Ba,^(144)Ce,and ^(147)Nd,and compared them with existing literature data to explore the energy dependence of fission products for ^(235)U.Given the lack of fission product yield data above 14.8 MeV,we extended our calculated incident neutron energy to 20 MeV,aiming to support future scientific research.The Geant4 physical model does not consider the influence of incident neutron energy on the average total kinetic energy of fission fragments;thus,we introduced the excitation function of the total kinetic energy of fission fragments recommended by Madland et al.,which effectively describes the experimental data of the average total kinetic energy of fragments formed in ^(235)U fission.In this paper,we comprehensively discuss the energy dependence of fission product yields and average total kinetic energy. 展开更多
关键词 ^^(235)u(n f) potential-driving model fission yields kinetic energies energy dependence
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Prompt fission neutron spectra of n+^(235)U above the(n,nf) fission threshold
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作者 舒能川 贾敏 +1 位作者 陈永静 刘挺进 《Chinese Physics C》 SCIE CAS CSCD 2015年第5期16-19,共4页
Calculations of prompt fission neutron spectra (PFNS) from the ^235U(n, f) reaction were performed with a semi-empirical method for En = 7.0 and 14.7 MeV neutron energies. The total PFNS were obtained as a superpo... Calculations of prompt fission neutron spectra (PFNS) from the ^235U(n, f) reaction were performed with a semi-empirical method for En = 7.0 and 14.7 MeV neutron energies. The total PFNS were obtained as a superposition of (n,xnf) pre-fission neutron spectra and post-fission spectra of neutrons which were evaporated from fission fragments, and these two kinds of spectra were taken as an expression of the evaporation spectrum. The contributions of (n,xnf) fission neutron spectra on the calculated PFNS were discussed. The results show that emission of one or two neutrons in the (n,nf) or (n,2nf) reactions influences the PFNS shape, and the neutron spectra of the (n,xnf) fission-channel are soft compared with the neutron spectra of the (n,f) fission channel. In addition, analysis of the multiple-chance fission component showed that second-chance fission dominates the PFNS with an incident neutron energy of 14.7 MeV whereas first-chance fission dominates the 7 MeV case. 展开更多
关键词 ^^235u(n f) neutron-induced fission prompt fission neutron spectrum
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Pre-neutron fragment mass yields for^(235)U(n,f)and^(239)Pu(n,f)reactions at incident energies from thermal up to 20 MeV
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作者 邹方磊 孙小军 +4 位作者 张凯 陈鸿飞 言杰 田俊龙 崔云怡 《Chinese Physics C》 SCIE CAS CSCD 2023年第4期161-167,共7页
Pre-neutron fragment mass yields in the vicinity of the thermal neutron energy are highly important for applications because of the larger fission cross sections of the^(235)U(n,f)and^(239)Pu(n,f)reactions.In this pap... Pre-neutron fragment mass yields in the vicinity of the thermal neutron energy are highly important for applications because of the larger fission cross sections of the^(235)U(n,f)and^(239)Pu(n,f)reactions.In this paper,preneutron fragment mass yields at incident energies from thermal up to 20 MeV are systematically studied using an empirical fission potential(EFP)model,the potential parameters of which are obtained from the measured data.The energy dependences of the peaks and valleys of the pre-neutron fragment mass yields are described by exponential and linear functions for the^(235)U(n,f)and^(239)Pu(n,f)reactions,respectively.The energy dependences of the evaporation neutrons,which play a crucial role in the reasonable description of pre-neutron fragment mass yields,are also obtained from the fission cross sections.The pre-neutron fragment mass yields in this study are not only consistent with the results of previous studies in regions of several Me Vs but also agree well with existing measured data at incident energies from thermal up to 20 MeV.The results show that the feasibility of this EFP model is verified in this extended energy region. 展开更多
关键词 ^^(235)u(n f)reaction ^^(239)Pu(n f)reaction thermal neutron energy empirical fission potential model pre-neutron fragment mass yield
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