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Fusion and quasifission studies for the ~(40)Ca + ~(186)W,~(192)Os reactions

机译:〜(40)Ca +〜(186)W,〜(192)OS反应的融合和促血管素研究

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Background: All elements above atomic number 113 have been synthesized using hot fusion reactions with calcium beams on statically deformed actinide target nuclei. Quasifission and fusion- fission are the two major mechanisms responsible for the very low production cross sections of superheavy elements. Purpose: To achieve a quantitative measurement of capture and quasifission characteristics as a function of beam energy in reactions forming heavy compound systems using calcium beams as projectiles. Methods: Fission fragment mass-angle distributions were measured for the two reactions ~(40)Ca+~(186)W and ~(40)C+~(192)Os, populating ~(226)Pu and ~(232)Cm compound nuclei, respectively, using the Heavy Ion Accelerator Facility and CUBE spectrometer at the Australian National University. Mass ratio distributions, angular distributions, and total fission cross sections were obtained from the experimental data. Simulations to match the features of the experimental mass-angle distributions were performed using a classical phenomenological approach. Results: Both ~(40)Ca+~(186)Wand ~(40)C+~(192)Os reactions showstrong mass-angle correlations at all energiesmeasured. A maximum fusion probability of 60−70% is estimated for the two reactions in the energy range of the present study. Coupled-channels calculations assuming standard Woods-Saxon potential parameters overpredict the capture cross sections. Large nuclear potential diffuseness parameters ~1.5 fm are required to fit the total capture cross sections. The presence of a weak mass-asymmetric quasifission component attributed to the higher angular momentum events can be reproduced with a shorter average sticking time but longer mass-equilibration time constant. Conclusions: The deduced above-barrier capture cross sections suggest that the dissipative processes are already occurring outside the capture barrier. The mass-angle correlations indicate that a compact shape is not achieved for deformation aligned collisions with lower capture barriers. The average sticking time of fast quasifission events is 10~(−20) s.
机译:背景:在静态变形的神经碱靶核上使用钙束的热熔反应合成了原子编号113的所有元素。 Quasifission和Fusion-裂变是两个主要机制,负责超效元素的极低生产横截面。目的:为了通过作为射弹形成重化合物系统的反应中的梁能量的函数的定量测量。方法:测量裂变片段质量分布的两种反应〜(40)Ca +〜(186)W和〜(40)C +〜(192)OS,填充〜(226)PU和〜(232)cm复合核分别在澳大利亚国立大学使用重离子加速器设施和立方体光谱仪。从实验数据中获得质量比分布,角度分布和总裂变横截面。使用经典的现象学方法进行匹配实验大分角分布的特征的模拟。结果:〜(40)CA +〜(186)棒〜(40)C +〜(192)OS反应在所有Energies训练中STRECTSTRONT阵切相关性。对于本研究能量范围的两种反应,估计了60-70%的最大融合概率。耦合通道计算假设标准木材 - 撒克逊潜在参数超出捕获横截面。适合总捕获横截面需要大核电相扩散参数〜1.5 FM。可以使用较短的平均粘附时间来再现归因于较高的角动量事件的弱的质量不对称Quasififififaction组件,但是较短的平均粘附时间,但较长的质量平衡时间常数。结论:推导出的上面禁区捕获横截面表明,耗散过程已经发生在捕获屏障之外。大分子角度相关表明,对于具有较低捕获屏障的变形对准的碰撞,不实现紧凑的形状。快速拟弧事件的平均粘附时间为10〜(--20)。

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  • 来源
    《Physical Review C》 |2017年第2017期|034608.1-034608.13|共13页
  • 作者单位

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia Department of Physics School of Mathematical and Physical Sciences Central University of Kerala Kasaragod 671314 India;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia Nuclear Physics Division Bhabha Atomic Research Centre Mumbai 400085 India.;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia Nuclear Physics Division Bhabha Atomic Research Centre Mumbai 400085 India.;

    Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

    National Superconducting Cyclotron Laboratory Michigan State University Michigan 48824 USA Department of Nuclear Physics Research School of Physical Sciences and Engineering Australian National University Canberra Australian Capital Territory 2601 Australia;

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