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arXiv 1408.3672physics.chem-ph
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氟分子F2的固定节点扩散蒙特卡罗potential energy曲线

Fixed-Node Diffusion Monte Carlo potential energy curve of the fluorine molecule F2 using selected configuration interaction trial wavefunctions

Emmanuel Giner, Anthony Scemama, Michel Caffarel

摘要:

采用组态相互作用(CI)型试探波函数,用固定节点扩散蒙特卡罗(FN-DMC)方法计算了F $_2$分子的势能曲线。为了保持行列式的数量合理(在FN-DMC的每一步都需要计算试探波函数的一阶和二阶导数),CI展开被限制在对总能量贡献最大的那些行列式上。决定因素的选择是使用所谓的CIPSI方法(使用迭代进行的扰动选择的配置交互)进行的。非常值得注意的是,CIPSI波函数的节点被发现是系统的改善时,增加所选择的行列式的数量。为了减少势能曲线的非平行性误差,引入了一种基于使用$R$依赖的行列式数的方案。数值结果表明,采用CIPSI试探波函数得到了F $_2$分子的改进的FN-DMC能量曲线.使用Dunning的cc-pVDZ基组,FN-DMC能量曲线的质量类似于使用FCI/cc-pVQZ获得的。在FN-DMC中使用所选CI的一个关键优点是可以以系统和自动的方式改进节点,而不需要像通常在FN-DMC中那样在变分蒙特卡罗水平上对试验波函数进行初步的多参数随机优化。

英文摘要:

The potential energy curve of the F$_2$ molecule is calculated with Fixed-Node Diffusion Monte Carlo (FN-DMC) using Configuration Interaction (CI)-type trial wavefunctions. To keep the number of determinants reasonable (the first and second derivatives of the trial wavefunction need to be calculated at each step of FN-DMC), the CI expansion is restricted to those determinants that contribute the most to the total energy. The selection of the determinants is made using the so-called CIPSI approach (Configuration Interaction using a Perturbative Selection made Iteratively). Quite remarkably, the nodes of CIPSI wavefunctions are found to be systematically improved when increasing the number of selected determinants. To reduce the non-parallelism error of the potential energy curve a scheme based on the use of a $R$-dependent number of determinants is introduced. Numerical results show that improved FN-DMC energy curves for the F$_2$ molecule are obtained when employing CIPSI trial wavefunctions. Using the Dunning's cc-pVDZ basis set the FN-DMC energy curve is of a quality similar to that obtained with FCI/cc-pVQZ. A key advantage of using selected CI in FN-DMC is the possibility of improving nodes in a systematic and automatic way without resorting to a preliminary multi-parameter stochastic optimization of the trial wavefunction performed at the Variational Monte Carlo level as usually done in FN-DMC.

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