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arXiv 0810.2996nucl-th
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偶-偶氩同位素的原子核结构及其磁矩

Nuclear Structure of the even-even Argon isotopes with a focus on magnetic moments

S. J. Q. Robinson, Y. Y. Sharon, L. Zamick

摘要:

我们研究了氩的重偶偶同位素中组态混合的作用。首先,我们将偶-偶Ar同位素的构型限定为$(d_{3/2}^2)_π$ $(f_{7/2}^n)_ν$。由于$^{40}$ Ar和$^{44}$ Ar在壳模型空间中的特殊位置,我们发现这两个核的能谱、B(E ~ 2)和磁矩是相同的。任何偏离这种相等性的情况都是构型混合的直接证据。在更大的壳模型空间中,这两种原子核之间存在显著差异,其中$^{44}$ Ar更具有集体性。我们还考虑了氩的其他偶偶同位素,并研究了它们的原子核结构效应如何随N的变化而变化。我们在全0 $\hbar ω$空间$(sd)_π$ $(fp)_ν$中比较了用WBT相互作用和用较新的SDPF(表示为SDPF-U)相互作用的计算结果。

英文摘要:

We study the role of configuration mixing in the heavier even-even isotopes of Argon. We begin by limiting the configurations of the even-even Ar isotopes to $(d_{3/2}^2)_π$ $(f_{7/2}^n)_ν$. There, due to the particular location in this shell model space of $^{40}$Ar and $^{44}$Ar, we find that the spectra, B(E2)'s and magnetic moments of these two nuclei are identical. Any deviation from this equality is direct evidence of configuration mixing. In a larger shell model space there are significant differences between these two nuclei, with $^{44}$Ar being more collective. We also consider other even-even isotopes of Argon and study how their nuclear structure effects evolve with N. We compare in the full 0$\hbar ω$ space $(sd)_π$ $(fp)_ν$ the results of calculations with the WBT interaction and with the newer SDPF, denoted SDPF-U, interaction.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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