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Neutron Emission in Fission And Quasi -Fissionof Hs

机译:裂变中的中子发射和Quasi -Fissionof

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Mass and energy distributions of fission -like fragments obtained in the reactions ~(26)Mg + ~(248)Cm, ~(36)S + ~(238)U and ~(58)Fe + ~(208)Pb leading to the formation of ~(266, 274)Hs are reported.From the analysis of TKE distributions for symmetric fragment it was found that at energies below the Coulomb barrier the bimodal fission of ~(274)Hs, formed in the reaction ~(26)Mg+~(248)Cm, is observed, while in the reaction ~(36)S+~(238)U at these energies the main part of the symmetric fragments arises from the quasi -fission process. At energies above the Coulomb barrier the fusion-fission is a main process leading to the formation of symmetric fragment for the both reactions. In the case of ~(58)Fe+~(208)Pb reaction the quasi-fission process is the main reaction mechanism at all measured energies. The pre- and post-scission neutron multiplicities as a function of the fragment mass have been obtained for all studied reactions.
机译:在反应中获得的裂变的裂变片段的质量和能量分布〜(26)Mg +〜(248)Cm,〜(36)S +〜(238)U和〜(58)Fe +〜(208)Pb通往报告了〜(266,274)HS的形成。从对称片段的TKE分布分析,发现在库仑屏障下方的能量〜(274)HS,反应中形成的双峰裂解〜(26)观察Mg +〜(248)厘米,而在反应中,在这些能量下,在这些能量下,对称片段的主要部分是从准碎片过程中出现的。在高于Coulomb屏障的能量,融合裂变是导致对称片段的两种反应形成的主要过程。在〜(58)Fe +〜(208)PB反应的情况下,准裂变过程是所有测量能量的主要反应机制。作为所有研究的反应,已经获得了作为片段质量的函数的裂变前和后的中子多重。

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