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arXiv 2207.07239nucl-th
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$^8$Be、$^{12}$C 和 $^{16}$O 系统中团簇运动的集体模型

Collective model for cluster motion in $^8$Be, $^{12}$C, and $^{16}$O systems

Yoshiko Kanada-En'yo, Nobuo Hinohara

AI总结:

该研究构建了基于微观团簇模型输入的集体模型,用于描述 $^8$Be、$^{12}$C 和 $^{16}$O 系统中基态和径向激发的团簇运动,并通过引入坐标虚部扩展模型,所得波函数与生成坐标法结果合理一致。

摘要:

将微观 $nα$ 团簇模型应用于 $^{8}$Be、$^{12}$C 和 $^{16}$O 系统,以研究基态和径向激发中的团簇运动。在使用生成坐标法并采用 $α$-$α$ 距离坐标 $D$ 对 $^{12}$C 和 $^{16}$O 进行微观计算时,激发态被获得为基于基态的大振幅模式。通过利用微观团簇模型的输入,如范数核和能量期望值,构建了一个集体模型来描述这些态的团簇运动。此外,通过引入坐标 $D$ 的虚部来扩展团簇模型,以纳入对集体质量的动力学效应。发现用集体模型获得的集体波函数在能量、均方根半径和振幅函数方面与生成坐标法的结果合理一致。

英文摘要:

A microscopic $nα$ cluster model was applied to $^{8}$Be, $^{12}$C, and $^{16}$O systems to investigate cluster motion in the ground state and radial excitation. In the microscopic calculation of $^{12}$C and $^{16}$O using the generator coordinate method with the coordinate $D$ of the $α$-$α$ distance, excited states were obtained as the large-amplitude mode built on the ground state. A collective model was constructed to describe the cluster motion of these states by utilizing inputs from the microscopic cluster model such as the norm kernel and energy expectation values. Furthermore, the cluster model was extended by introducing the imaginary part of the coordinate $D$ to incorporate the dynamical effects on the collective mass. The collective wave function obtained with the collective model was found to be in reasonable agreement with the results of the generator coordinate method for energies, root-mean-square radii, and amplitude functions.

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