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Effect of Nuclear-Reaction Mechanisms on the Population of Excited Nuclear States and Isomeric Ratios

机译:核反应机制对核兴奋态人口和同构比率的影响

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Experimental data on the cross sections for channels of fusion and transfer reactions induced by beams of radioactive halo nuclei and clustered and stable loosely bound nuclei were analyzed, and the results of this analysis were summarized. The interplay of the excitation of single-particle states in reaction-product nuclei and direct reaction channels was established for transfer reactions. Respective experiments were performed in stable (Li-6) and radioactive (He-6) beams of the DRIBs accelerator complex at the Flerov Laboratory of Nuclear Reactions, Joint Institute for Nuclear Research, and in deuteron and He-3 beams of the U-120M cyclotron at the Nuclear Physics Institute, Academy Sciences of Czech Republic (Rez and Prague, Czech Republic). Data on subbarrier and near-barrier fusion reactions involving clustered and loosely bound light nuclei (Li-6 and He-3) can be described quite reliably within simple evaporation models with allowance for different reaction Q-values and couple channels. In reactions involving halo nuclei, their structure manifests itself most strongly in the region of energies below the Coulomb barrier. Neutron transfer occurs with a high probability in the interactions of all loosely bound nuclei with light and heavy stable nuclei at positive Q-values. The cross sections for such reactions and the respective isomeric ratios differ drastically for nucleon stripping and nucleon pickup mechanisms. This is due to the difference in the population probabilities for excited single-particle states.
机译:分析了由放射性晕核束和聚集且稳定的松散结合核束诱导的融合和转移反应通道截面的实验数据,并总结了分析结果。建立了反应产物核和直接反应通道中单粒子态激发的相互作用,以进行转移反应。在联合核研究所弗莱罗夫核反应实验室的DRIBs加速器复合物的稳定(Li-6)和放射性(He-6)光束中,以及在U-捷克共和国科学院(雷兹和布拉格)捷克核物理研究所的120M回旋加速器。在简单的蒸发模型中,考虑到不同的反应Q值和耦合通道,可以非常可靠地描述涉及成簇和松散结合的轻核(Li-6和He-3)的亚势垒和近势垒聚变反应的数据。在涉及卤原子核的反应中,它们的结构在库仑势垒以下的能量区域中最明显地表现出来。在正Q值下,所有松散结合的原子核与轻,重的稳定核相互作用时,中子转移的可能性很高。对于核子剥离和核子拾取机制,此类反应的横截面和相应的异构体比率截然不同。这是由于激发的单粒子状态的总体概率不同。

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