论文标题

$^{129} Xe+^{nat} sn $ from $ 8a $ $ $ mev $最高$ 18A $ $ MEV $和$^{129} xe+^{197} au $ 15a $ 15a $ meV $和$ 18A $ $ MEV $ $ 18A

Analysis of 2-Body Central Events for $^{129}Xe+^{nat}Sn$ from $8A$ $MeV$ up to $18A$ $MeV$ and for $^{129}Xe+^{197}Au$ at $15A$ $MeV$ and $18A$ $MeV$

论文作者

Manduci, L., Lopez, O., Durand, D., Bougault, R., Vient, E., Pâlog, M., Borderie, B., Lombardo, I., Verde, G.

论文摘要

提出了一项对导致从屏障到18A MEV的出口通道中两个碎片的中质量重离子反应的研究。对于所选的出口通道中的两个片段($ z \ geq10 $)的事件,将特别的重点放在裂变和准叶片上。 $^{129} XE $ prackiles在$^{nat} sn $上以及$^{197} au au $ in Energies上引起的反应,分析了$ 8A $ MEV到$ 18A $ MEV。使用等于2的片段($ z \ geq10 $)多重性,使用裂变片段电荷分布,总体动能分布(TKE)及其标准偏差$σ__{TKE} $,研究了最低光束能量的裂变和准裂变事件。对于较轻的系统,仍然可以观察到不完全融合的裂变事件。在差异方面,对于较重的系统,可以证明金靶上的氙气仅证明了准膜。对最终通道中两个片段的事件的研究表明,与入口通道中的融合有关的裂变在两个系统的20A MEV左右消失。在较低的能量(8A,12A和15A MEV)的SN目标下,在片段电荷分布中显示出具有越来越大能量的进化。这种趋势可以归因于增长的角动量,如光电荷颗粒的平面外部分布所表明的那样。在15A MEV的黄金靶情况下,也观察到相同的效果。但是,对于这个较重的系统,可以证明对导致准裂缝的入口通道的强烈记忆。此外,与中提琴系统的比较显示出一个偏差,对于$^{129} Xe+^{nat} sn $ System的偏重。对上述结果的完整了解肯定需要在这些能量上进行精确的模型计算。

A study of medium-mass heavy-ion reactions leading to two fragments in the exit channel from barrier to 18A MeV is proposed. A special focus is made on fission and quasi-fission for events with two fragments ($Z\geq10$) in the exit channel selected. Reactions induced by $^{129}Xe$ projectiles on $^{nat}Sn$ and on $^{197}Au$ at energies ranging from $8A$ MeV to $18A$ MeV were analyzed. Using the fragment ($Z\geq10$) multiplicity equal to 2, fission and quasi-fission events were studied for the lowest beam energies using the fission fragment charge distributions, the total kinetic energy distribution (TKE) and its standard deviation $σ_{TKE}$. For the lighter system it is still possible to observe fission events from incomplete fusion. At variance, for the heavier system, Xenon on gold target only quasi-fission is evidenced. The study of the events characterized by two fragments in the final channel shows that fission, related to fusion in the entrance channel, disappears around 20A MeV for both systems. At lower energies (8A, 12A and 15A MeV) for the Sn target, an evolution with increasing energies towards an asymmetric fission mode is displayed in the fragment charge distributions. This trend can be attributed to the increasing angular momentum as indicated by the out-of-plane angular distribution for light charged particles. The same effect is also observed in the case of the gold target at 15A MeV. However, for this heavier system, a strong memory of the entrance channel leading to quasi-fission is evidenced. A comparison with the Viola systematics, moreover, shows a deviation, greater for the heavier system than for $^{129}Xe+^{nat}Sn$ system. A complete understanding of the above results would certainly require precise model calculations at these energies.

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