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A Deterministic Projector Configuration Interaction Approach for the Ground State of Quantum Many-Body Systems

机译:量子多体系统基态的确定性投影仪配置相互作用方法

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In this work we propose a novel approach to solve the Schrodinger equation which combines projection onto the ground state with a path-filtering truncation scheme. The resulting projector configuration interaction (PCI) approach realizes a deterministic version of the full configuration interaction quantum Monte Carlo (FCIQMC) method [Booth, G. H.; Thom, A. J. W.; Alavi, A. J. Chem. Phys. 2009, 131, 054106]. To improve upon the linearized imaginary-time propagator, we develop an optimal projector scheme based on an exponential Chebyshev expansion in the limit of an infinite imaginary time step. After writing the exact projector as a path integral in determinant space, we introduce a path filtering procedure that truncates the size of the determinantal basis and approximates the Hamiltonian. The path filtering procedure is controlled by one real threshold that determines the accuracy of the PCI energy and is not biased toward any determinant. Therefore, the PCI approach can equally well describe static and dynamic electron correlation effects. This point is illustrated in benchmark computations on N-2 at both equilibrium and stretched geometries. In both cases, the PCI achieves chemical accuracy with wave functions that contain less than 0.5% determinants of full CI space. We also: report computations on the ground state of C-2 with up to quaduple-zeta basis sets and wave functions as large as 200 million determinants, which allow a direct comparison of the PCI, FCIQMC, and density matrix renormalization group (DMRG) methods. The size of the PCI wave function grows modestly with the number of unoccupied orbitals, and its accuracy maybe tuned to match that of FCIQMC and DMRG.
机译:在这项工作中,我们提出了一种新颖的方法来求解薛定inger方程,该方程将路径投影到截断方案结合到基态上。最终的投影仪配置交互(PCI)方法实现了完整配置交互量子蒙特卡洛(FCIQMC)方法的确定性版本[Booth,G. H .; Thom,A. J. W .; Alavi,A.J.Chem。物理2009,131,054106]。为了改进线性化的虚时传播器,我们在无限虚时间步长的限制下,基于指数切比雪夫展开,开发了一种最佳的投影仪方案。在将确切的投影机写为行列式空间中的路径积分后,我们引入了一个路径滤波过程,该过程将截去行列式基础的大小并近似哈密顿量。路径过滤过程由确定PCI能量精度的一个实际阈值控制,并且不偏向任何决定因素。因此,PCI方法可以很好地描述静态和动态电子相关效应。在平衡几何和拉伸几何中,N-2的基准计算都说明了这一点。在这两种情况下,PCI的波函数都包含小于全部CI空间决定因素的0.5%,从而达到了化学精度。我们还:报告C-2的基态计算,具有多达四倍的Zeta基集和高达2亿行列式的波动函数,从而可以直接比较PCI,FCIQMC和密度矩阵重归一化组(DMRG)方法。 PCI波函数的大小随未占用的轨道数而适度增长,并且其精度可以调整为与FCIQMC和DMRG相匹配。

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