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RELATIVISTIC MEAN-FIELD THEORY ON THE XENON, CESIUM AND BARIUM ISOTOPES

机译:氙,铯和钡同位素的相对论均值理论

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摘要

We apply the relativistic mean-field theory to unstable nuclei with Z = 54, 55 and 56. We compare the results of calculations to experimental data of the mean-square-charge radii and binding energies using the parameter set, TM1. The constraint calculations result in an energy curve as a function of deformation with several candidates for the absolute minimum for each nucleus. The strong shell effect at N = 82, for the Xe and Ba isotopes is clearly observed in the present theory, but for Cs isotopes the effect is not so drastic, which is in good agreement with experimental observation. The energy minimum at large prolate deformation, which appears at the proton-rich side, can explain the jump of the mean-square-charge radius at N similar to 64 for the Cs isotopes. [References: 26]
机译:我们将相对论平均场理论应用于Z = 54、55和56的不稳定核。我们使用参数集TM1将计算结果与均方电荷半径和结合能的实验数据进行比较。约束计算得出的能量曲线是变形的函数,每个原子核的绝对最小值有几个候选值。在本理论中,对于Xe和Ba同位素在N = 82时有很强的壳层效应,但是对于Cs同位素而言,这种效应并不那么剧烈,这与实验观察结果非常吻合。扁长形大变形处的最小能量出现在富质子侧,可以解释Cs同位素在N处的均方电荷半径的跃迁,类似于64。 [参考:26]

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