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Momentum space calculations of the binding energies of argon dimer

机译:氩水二聚体绑定能量的动量空间计算

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The binding energies of argon dimer are calculated by solving the homogeneous Lippmann-Schwinger integral equation in momentum space. Our numerical analysis using two models of argon-argon interaction developed by Patkowski et al. not only confirms the eight argon dimer vibrational levels of the ground state of argon dimer (ie, for j = 0) predicted by other groups but also provides a very precise means for determining the binding energy of the ninth state which its value is a matter of discussion. Our calculations have been also extended to states with higher rotational quantum number j and we have calculated the energy of all 174 bound states for both potential models. Our numerical results for vibrational levels of the ground state of argon dimer are in excellent agreement with other theoretical calculations and available experimental data.
机译:通过在动量空间中求解均匀的Lippmann-Schwinger整体方程来计算氩二聚体的结合能量。 我们使用Patkowski等人开发的两种氩氩互动模型的数值分析。 不仅确认由其他组预测的氩正式的地面状态的八个氩水二聚体振动水平(即,对于J = 0),还提供了非常精确的装置,用于确定其值是物质的第九状态的绑定能量 讨论。 我们的计算也扩展到具有更高旋转量子数J的状态,我们已经计算了所有174个界定状态的能量,适用于两个潜在模型。 我们对氩气二聚体的地面状态的振动水平的数值结果与其他理论计算和可用的实验数据非常一致。

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