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A new near-linear scaling, efficient and accurate, open-shell domain-based local pair natural orbital coupled cluster singles and doubles theory

机译:一种新的近线性缩放,高效准确,基于壳域的本地对自然轨道耦合集群单打和双打理论

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The Coupled-Cluster expansion, truncated after single and double excitations (CCSD), provides accurate and reliable molecular electronic wave functions and energies for many molecular systems around their equilibrium geometries. However, the high computational cost, which is well-known to scale as O(N-6) with system size N, has limited its practical application to small systems consisting of not more than approximately 20-30 atoms. To overcome these limitations, low-order scaling approximations to CCSD have been intensively investigated over the past fewyears. In our previous work, we have shown that by combining the pair natural orbital (PNO) approach and the concept of orbital domains it is possible to achieve fully linear scaling CC implementations (DLPNO-CCSD and DLPNO-CCSD(T)) that recover around 99.9% of the total correlation energy [C. Riplinger et al., J. Chem. Phys. 144, 024109 (2016)]. The production level implementations of the DLPNO-CCSD and DLPNO-CCSD(T) methods were shown to be applicable to realistic systems composed of a few hundred atoms in a routine, black-box fashion on relatively modest hardware. In 2011, a reduced-scaling CCSD approach for high-spin open-shell unrestricted Hartree-Fock reference wave functions was proposed (UHF-LPNO-CCSD) [A. Hansen et al., J. Chem. Phys. 135, 214102 (2011)]. After a few years of experience with this method, a few shortcomings of UHF-LPNO-CCSD were noticed that required a redesign of the method, which is the subject of this paper. To this end, we employ the high-spin open-shell variant of the N-electron valence perturbation theory formalism to define the initial guess wave function, and consequently also the open-shell PNOs. The new PNO ansatz properly converges to the closed-shell limit since all truncations and approximations have been made in strict analogy to the closed-shell case. Furthermore, given the fact that the formalism uses a single set of orbitals, only a single PNO integral transformation is necessary, which offers large computational savings. We show that, with the default PNO truncation parameters, approximately 99.9% of the total CCSD correlation energy is recovered for open-shell species, which is comparable to the performance of the method for closed-shells. UHF-DLPNO-CCSD shows a linear scaling behavior for closed-shell systems, while linear to quadratic scaling is obtained for open-shell systems. The largest systems we have considered contain more than 500 atoms and feature more than 10 000 basis functions with a triple-zeta quality basis set. Published by AIP Publishing.
机译:单一和双激发(CCSD)之后截断的耦合簇扩展为许多围绕其平衡几何形状提供了准确可靠的分子电子波功能和能量。然而,具有众所周知的具有系统尺寸N的高计算成本,其具有系统尺寸N的o(n-6),其实际应用于由不超过大约20-30个原子组成的小系统。为了克服这些限制,在过去的少年中,对CCSD的低阶缩放近似是集中的。在我们以前的工作中,我们已经表明,通过组合对自然轨道(PNO)方法以及轨道域的概念,可以实现恢复的完全线性缩放CC实现(DLPNO-CCSD和DLPNO-CCSD(T))总相关能量的99.9%[C. Riplinger等人。,J.Chem。物理。 144,024109(2016)]。 DLPNO-CCSD和DLPNO-CCSD(T)方法的生产水平实现显示,适用于在相对适度的硬件上的例程中由一百个原子组成的现实系统。 2011年,提出了一种减少的高自旋开壳不受限制的Hartree-Fock参考波函数的CCSD方法(UHF-LPNO-CCSD)[A. Hansen等人。,J.Chem。物理。 135,214102(2011)]。经过几年的经验解决这种方法,注意到UHF-LPNO-CCSD的一些缺点被注意到需要重新设计该方法,这是本文的主题。为此,我们采用N-Electron Vencencation Percurbation理论形式主义的高自旋开壳变型来定义初始猜测波函数,因此也是开放式壳体PNO。新的PNO ANSATZ适当地收敛到闭合壳限制,因为所有截断和近似都是严格地对闭式壳盒进行的。此外,鉴于形式主义使用单组轨道的事实,只有单个PNO积分转换是必要的,这提供了大的计算储蓄。我们展示了,通过默认的PNO截断参数,对于开壳物种,大约99.9%的CCSD相关能量恢复,这与闭合壳方法的性能相当。 UHF-DLPNO-CCSD为闭带系统表示线性缩放行为,而对于开壳系统,可以获得与二次缩放的线性。我们考虑的最大系统包含超过500个原子,并具有超过10 000个基础函数,具有三级Zeta质量基础集。通过AIP发布发布。

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