共查询到20条相似文献,搜索用时 140 毫秒
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用5.5到21.7MeV/A28Si+197Au,测量关联裂片的速度及角分布.实验表明:入射能超过10MeV/A时,出现非完全熔合裂变(ICF);Ecm>200MeV时,伴随ICF又出现跟随裂变(SF).从线性动量转移(LMT)分布中,提取了SF产额对总裂变产额的比值.从关联裂片偏离反应平面的分布中,给出了分布宽度与单核子激发能的线性关系式. 相似文献
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对132MeV 16O+197Au反应产生的裂变碎片和巨偶极共振γ射线进行了符合测量,得到了E=92MeV的高激发213Fr的γ衰变谱和γ角关联谱.观测到复合核巨偶极共振γ角关联谱存在很大的各向异性.利用改进的统计模型程序分析了实验数据,不考虑裂变延迟时,统计模型计算可以很好拟合地实验结果.通过对γ角关联谱的理论计算与实验结果的比较,可以得出高激发213Fr核(E=92MeV)的形状从集体长椭球向非集体扁椭球变化. 相似文献
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在25MeV/u 40Ar+natAg、209Bi反应中,用4个PPAC和11组望远镜完成了关联裂变碎片与发射轻粒子的符合测量,角关联描绘为两个被探测到碎片折叠角θff的函数,线性动量转移〈LMT〉由测量到的角关联推出.将符合测量得到的对应于不同窗的后角轻带电粒子能谱用Maxwell分布来拟合其谱的后沿,经过一些修正,由能谱得到热核的初始温度Tint,在考虑反应Q值和预平衡发射的修正之后,可以得到不同窗所对应的激发能.实验结果表明,在40Ar+natAg、209Bi反应的中心碰撞中激发能分别为4.2、2.4MeV/u,而温度达6.1、5.5MeV,在半中心碰撞中激发能为3.5、1.9MeV/u,温度可达5.8、4.8MeV. 相似文献
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The prompt fission neutron spectra for the neutron-induced fission of 233U for low energy neutrons (below 6 MeV) are calculated using nuclear evaporation theory with a semi-empirical method, in which the partition of the total excitation energy between the fission fragments for the nth+233U fission reactions is determined by the available experimental and evaluation data. The calculated prompt fission neutron spectra agree well with the experimental data. The proportions of high-energy neutrons of prompt fission neutron spectrum versus incident neutron energies are investigated with the theoretical spectra, and the results are consistent with the systematics. The semi-empirical method could be a useful tool for the prompt evaluation of fission neutron spectra. 相似文献
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For the n+<'235>U fission reaction, the total excitation energy partition of the fission fragments, the average neutron kinetic energy <ε>(A) and the total average energies E<,γ>(A) removed by γ rays as a function of fission fragment mass are given at incident energies up to 20 MeV. The prompt neutron multiplicity as a function of the fragment mass, ν(A), for neutron-induced fission of <'235>U at different incident neutron energies is calculated. The calculated results are checked with the total average prompt neutron multiplicities ν and compared with the experimental and evaluated data. Some prompt neutron and γ emission mechanisms are discussed. 相似文献
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E.A. Zhagrov I.M. Kuks Yu.A. Nemilov Yu.A. Selitskii V.B. Funstein 《Nuclear Physics A》1973,213(3):436-444
Kinetic energy spectra of fragments in the 5–15 MeV neutron-induced fission of 226Ra are obtained. The fraction of fragments corresponding to the central peak of the mass yield curve is determined for each neutron energy used. It is shown that at low excitation energies of the 227Ra compound nucleus precluding second-chance fission the mass yield curve retains its triple-peaked nature. At still lower excitations, near the fission threshold, radium undergoes asymmetric fission, just as the heavier nuclei. 相似文献
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Low energy neutron induced fission of ~(235)U is studied in the framework of the multi-modal fission model. The fission fragment properties, such as the yields, the average total kinetic energy distribution and the average neutron separation energy, are investigated for incident neutron energies from thermal to 6.0 MeV. The multi-modal fission approach is also used to evaluate the prompt fission neutron multiplicity and spectra for the neutron-induced fission of ~(235)U with an improved version of the Los Alamos model for incident neutrons below the (n, nf) threshold. The three most dominant fission modes are taken into account. The model parameters are determined on the basis of experimental data. The calculated results are in good agreement with the experimental data. 相似文献
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According to some experimental and evaluated data, the total excitation energy partitioning way between both of the fission fragments was given with a semi-empirical method. With the calculated energy partitioning way, the prompt neutron multiplicity as a function of fragment mass, (-v)(A), for neutron-induced fission of 235U at En=0.0253 eV, 3 MeV, and 5 MeV was calculated. The results are checked with the total average prompt neutron multiplicities (-v) and compared with the experimental and evaluated data. 相似文献
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V. A. Drozdov D. O. Eremenko O. V. Fotina S. Yu. Platonov O. A. Yuminov 《Physics of Atomic Nuclei》2003,66(9):1628-1630
The unified energy dependence of the induced fission times obtained by the crystal blocking technique for heavy nuclei with Z=91–94 in the range of initial excitation energy from 5 to 250 MeV was analyzed. It was demonstrated that, for excitation energies of the investigated heavy fissionable nuclei up to 60–70 MeV, the fission times can be described in the framework of the statistical theory of nuclear reactions taking into account the double-humped structure of the fission barrier and the lifetimes of both classes of excited nuclear states realized in the first and second potential wells. However, for excitation energies above 70 MeV, there is a need to consider the dynamical effects in the fission channel. 相似文献
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The recoil properties of ten fission products with masses ranging from 72 to 136 formed in the fission of 238U with protons of energies 25–85 MeV have been determined radiochemically by the integral-range method. From the recoil properties of the products and the Monte Carlo cascade calculations the average kinetic energy, cascade deposition energy, and anisotropy parameter for each fission product has been calculated. The kinetic energy and the excitation energy of the primary fragments leading to the observed fission product, and the total kinetic energy and the total excitation energy of the primary fragment pair have also been calculated.
The results indicate that up to a bombarding energy of 40 MeV fission takes place predominantly by the compound nucleus mechanism, with an increasing contribution of the direct interaction mechanism as the bombarding energy increases. The kinetic energy deficit was found to decrease with increasing bombarding energy. The fission products formed from the symmetric mode of fission have a larger separation distance between the charge centres of their respective primary fragments than those for the asymmetric mode of fission. 相似文献
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J. Van Der Plicht M.N. Harakeh A. Van Der Woude P. David J. Debrus H. Janszen J. Schulze 《Nuclear Physics A》1981,369(1):51-76
The fission probabilities and angular distributions of the fission fragments for the (α, α'f) reaction on 232Th and 238U at a bombarding energy of 120 MeV have been measured from about 4 to 14 MeV excitation energy. Evidence for sub-barrier resonances has been found, the negativeparity ones occurring at the same excitation energy where photofission resonances have been observed. The data are analyzed with the two-humped barrier model. For 238U the data are reasonably well fitted with barriers similar to those known from the literature. For 232Th though, the outer barrier parameters are quite different: the height EB = 6.6 MeV and the width (khω)B = 1.2 MeV. Also for 232Th, introducing an additional mass symmetric and axially asymmetric outer barrier, as was previously found necessary for 238U, does not result in a good fit to the data at higher excitation energies. 相似文献
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LI Jia-Xing LIU Ping-Ping WANG Jian-Song HU Zheng-Guo MAO Aui-Shi SUN Zhi-Yu LI Chen CHEN Ruo-Fu XU Hu-Shan XIAO Guo-Qing GUO Zhong-Yan 《中国物理C(英文版)》2010,34(4)
The mirror nuclei ~(12)N and ~(12)B are separated by the Radioactive Ion Beam Line in Lanzhou (RIBLL)at HIRFL from the breakup of 78.6 MeV/u ~(14)N on a Be target. The total reaction cross-sections of ~(12)N at 34.9 MeV/u and ~(12)B at 54.4 MeV/u on a Si target have been measured by using the transmission method.Assuming ~(12)N consists of a ~(11)C core plus one halo proton, the excitation function of ~(12)N and ~(12)B on a Si target and a C target were calculated with the Glauber model. It can fit the experimental data very well. The characteristic halo structure for ~(12)N was found with a large diffusion of the protons density distribution. 相似文献
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Low energy neutron induced fission of 235U is studied in the framework of the multi-modal fission model. The fission fragment properties, such as the yields, the average total kinetic energy distribution and the average neutron separation energy, are investigated for incident neutron energies from thermal to 6.0 MeV. The multi-modal fission approach is also used to evaluate the prompt fission neutron multiplicity and spectra for the neutron-induced fission of 235U with an improved version of the Los Alamos ... 相似文献