Explicitly correlated trial wavefunctions in quantum Monte Carlo calculations of excited states of Be and Be

L. Bertini, D. Bressanini, M. Mella, G. Morosi
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引用次数: 13

Abstract

We present a new form of explicitly correlated wavefunction whose parameters are mainly linear, to circumvent the problem of the optimization of a large number of nonlinear parameters usually encountered with basis sets of explicitly correlated wavefunctions. With this trial wavefunction we have succeeded in minimizing the energy instead of the variance of the local energy, as is more common in quantum Monte Carlo methods. We have applied this wavefunction to the calculation of the energies of Be 3 P (1s 2 2p 2 ) and Be − 4 S o (1s 2 2p 3 ) by variational and diffusion Monte Carlo methods. The results compare favourably with those obtained by different types of explicitly correlated trial wavefunction already described in the literature. The energies obtained are improved with respect to the best variational ones found in the literature, and within one standard deviation of the estimated non-relativistic limits.
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量子蒙特卡罗计算中Be和Be激发态的显式相关试验波函数
本文提出了一种参数以线性为主的显式相关波函数的新形式,避免了显式相关波函数基集通常遇到的大量非线性参数的优化问题。利用这个试验波函数,我们成功地使能量最小化,而不是使局部能量的方差最小化,这在量子蒙特卡罗方法中更为常见。我们用变分和扩散蒙特卡罗方法计算了Be 3p (1s 2 2p 2)和Be - 4s o (1s 2 2p 3)的能量。所得结果与文献中描述的不同类型的显式相关试验波函数所得的结果相吻合。得到的能量相对于文献中发现的最佳变分能量有所改进,并且在估计的非相对论性极限的一个标准差内。
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