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arXiv 0906.0880nucl-thnucl-ex
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PDMATHAAB S+ $^{182,184}$ W反应中聚变- fission与准裂变过程的竞争

Competition between fusion-fission and quasifission processes in the $^{32}$S+$^{182,184}$W reactions

H. Q. Zhang, C. L. Zhang, C. J. Lin, Z. H. Liu, F. Yang, A. K. Nasirov, G. Mandaglio, M. Manganaro, G. Giardina

摘要:

测量了质心能量为118.8、123.1、127.3、131.5、135.8、141.1和144.4 MeV的$^{32}$ S+ $^{184}$ W反应的裂变碎片角分布。得到了实验裂变激发函数。通过外推各裂变角分布,得到了碎片角各向异性($\mathcal{A}_{\rm exp}$)。用双核系统模型将测量的$^{32}$ S+ $^{182,184}$ W反应的裂变截面分解为聚变裂变、准裂变和快裂变的贡献。在先进的统计模型的框架下计算的$^{32}$ S+ $^{184}$ W反应的总蒸发残渣激发函数与现有的实验数据符合良好,直到约$E_{\rm c.m.}\approx 160$ MeV。在所考虑的束能量范围内,用相同的部分俘获截面对反应和表征裂变产物角分布的量$K_0^2$、$<\ell^2>$和$\mathcal{A}_{\rm exp}$的实验俘获激发函数进行了理论描述。

英文摘要:

The angular distributions of fission fragments for the $^{32}$S+$^{184}$W reaction at center-of-mass energies of 118.8, 123.1, 127.3, 131.5, 135.8, 141.1 and 144.4 MeV were measured. The experimental fission excitation function is obtained. The fragment angular anisotropy ($\mathcal{A}_{\rm exp}$) is found by extrapolating the each fission angular distributions. The measured fission cross sections of the $^{32}$S+$^{182,184}$W reaction are decomposed into fusion-fission, quasifission and fast fission contributions by the dinuclear system model. The total evaporation residue excitation function for the $^{32}$S+$^{184}$W reaction calculated in the framework of the advanced statistical model is in good agreement with the available experimental data up to about $E_{\rm c.m.}\approx 160$ MeV. The theoretical descriptions of the experimental capture excitation functions for both reactions and quantities $K_0^2$, $<\ell^2>$ and $\mathcal{A}_{\rm exp}$ which characterize angular distributions of the fission products were performed by the same partial capture cross sections at the considered range of beam energy.

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