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Local Correlation Calculations Using Standard and Renormalized Coupled-Cluster Methods

机译:使用标准和重字耦合群集方法的本地相关性计算

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This article discusses our recent effort toward the extension of the linear scaling local correlation approach, termed 'cluster-in-molecule' and abbreviated as CIM [S. Li, J. Ma, and Y. Jiang, Comput. Chem. 23, 237 (2002); S. Li, J. Shen, W. Li, and Y. Jiang, Chem. Phys. 125, 074109 (2006)1 to the coupled-cluster (CC) theory with singles and doubles (CCSD) and CC methods with singles, doubles, and non-iterative triples, including the standard CCSD(T) approach and the completely renormalized CR-CC(2,3) scheme [P. Piecuch and M. W/och, J. Chem. Phys. 123, 224105 (2005); P. Piecuch, M. Wloch, J.R. Gour, and A. Kinal, Chem. Phys. Lett. 418, 467 (2006)]. As in the earlier CIM work that dealt with the second-order many-body perturbation theory and CC doubles approach, the main idea of the CIM-CCSD, CIM-CCSD(T), and CIM-CR-CC(2,3) methods is the realization of the fact that the total correlation energy of a large system can be obtained as a sum of contributions from the occupied orthonormal localized molecular orbitals and their respective occupied and unoccupied orbital domains. The CIMCCSD, CIM-CCSD(T), and CIM-CR-CC(2,3) methods pursued in this work are characterized by high computational efficiency in both the CIM and CC parts, enabling calculations for much larger systems than previously possible. This is achieved by combining the natural linear scaling and embarrassing parallelism of the CIM ansatz with the vectorized CC codes that rely on recursively generated intermediates and fast matrix multiplication routines. By comparing the results of the canonical and CIM-CC calculations for normal alkanes and water clusters, it is demonstrated that the CIM-CCSD, CIM-CCSD(T), and CIM-CR-CC(2,3) approaches recover the corresponding canonical CC correlation energies to within 0.1 % or so, while offering linear scaling of the computer costs with the systeth size and savings in the computer effort by orders of magnitude. By examining the dissociation of dodecane into C 1 1H23 and CH3 and several lowest-energy structures of the (H 20)clusters, it is shown that the CIM-CC methods accurately reproduce the relative energetics of the corresponding canonical CC calculations.
机译:本文讨论了我们最近努力扩展线性缩放局部相关方法,称为“分子集群”并缩写为CIM [S.李,J.Ma和Y.江,计算。化学。 23,237(2002); S. Li,J. Shen,W. Li,Zhen,Chem。物理。 125,074109(2006)1与单打和双打(CCSD)和CC方法的耦合集群(CC)理论,具有单打,双打和非迭代三元组,包括标准CCSD(T)方法和完全称为称为CR -CC(2,3)计划[P. Piquch和M. w / Och,J.Chem。物理。 123,224105(2005); P.Imuch,M.Wloch,J.R. Gour和A.Kinal,Chem。物理。吧。 418,467(2006)]。如在早期的CIM工作中处理二阶许多扰动理论和CC双打方法,CIM-CCSD,CIM-CCSD(T)和CIM-CR-CC(2,3)的主要思想方法是实现大型系统的总相关能量可以获得作为来自占用的正交分子分子轨道的贡献的总和及其各自的占用和未占用的轨道结构域。在该工作中追求的CIMCCSD,CIM-CCSD(2,3)方法的特点是CIM和CC零件中的高计算效率,使得能够计算比以前更大的系统。这是通过将CIM Ansatz的自然线性缩放和令人尴尬的平行性与依赖于递归生成的中间体和快速矩阵乘法例程的速率相结合来实现的实现。通过比较正常烷烃和水簇的规范和CIM-CC计算的结果,证明CIM-CCSD,CIM-CCSD(T)和CIM-CR-CC(2,3)接近相应的方法规范CC相关能量在0.1%左右的情况下,同时通过Systeve尺寸提供计算机成本的线性缩放,并按照级别节省计算机努力。通过将十二烷的解离进入C 1 1H23和CH3和几个(H 20)簇的几个最低能量结构,示出了CIM-CC方法精确地再现了相应的规范CC计算的相对能量。

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