首页> 外文期刊>The Journal of Chemical Physics >DENSITY FUNCTIONAL RESULTS FOR ISOTROPIC AND ANISOTROPIC MULTIPOLE POLARIZABILITIES AND C-6, C-7, AND C-8 VAN DER WAALS DISPERSION COEFFICIENTS FOR MOLECULES
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DENSITY FUNCTIONAL RESULTS FOR ISOTROPIC AND ANISOTROPIC MULTIPOLE POLARIZABILITIES AND C-6, C-7, AND C-8 VAN DER WAALS DISPERSION COEFFICIENTS FOR MOLECULES

机译:分子的各向同性和各向异性多极化和C-6,C-7和C-8范德华扩散系数的密度泛函结果

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The generalized gradient-approximated (GGA) energy functionals used in density functional theory (DFT) provide accurate results for many different properties. However, one of their weaknesses lies in the fact that Van der Waals forces are not described. In spite of this, it is possible to obtain reliable long-range potential energy surfaces within DFT. In this paper, we use time-dependent density functional response theory to obtain the Van der Waals dispersion coefficients C-6, C-7, and C-8 (both isotropic and anisotropic). They are calculated from the multipole polarizabilities at imaginary frequencies of the two interacting molecules. Alternatively: one might use one of the recently-proposed Van der Waals energy functionals for well-separated systems, which provide fairly good approximations to our isotropic results. Results with the local density approximation (LDA), Becke-Perdew (BP) GGA and the Van Leeuwen-Baerends (LB94) exchange-correlation potentials are presented for the multipole polarizabilities and the dispersion coefficients of several rare gases, diatomics and the water molecule. The LB94 potential clearly performs best, due to its correct Coulombic asymptotic behavior, yielding results which are close to those obtained with many-body perturbation theory (MBPT). The LDA and BP results are systematically too high for the isotropic properties. This becomes progressively worse for the higher dispersion coefficients. The results for the relative anisotropies are quite satisfactory for all three potentials, however. (C) 1997 American Institute of Physics. [References: 54]
机译:密度泛函理论(DFT)中使用的广义梯度近似(GGA)能量泛函为许多不同的性质提供了准确的结果。然而,它们的弱点之一在于没有描述范德华力。尽管如此,仍可以在DFT中获得可靠的远距离势能面。在本文中,我们使用时变密度函数响应理论来获得范德华分散系数C-6,C-7和C-8(各向同性和各向异性)。它们是根据两个相互作用分子的假想频率处的多极极化率计算的。另一种方法是:对于分离良好的系统,可以使用最近提出的Van der Waals能量函数之一,该函数可以很好地近似我们的各向同性结果。给出了局部密度近似(LDA),Becke-Perdew(BP)GGA和Van Leeuwen-Baerends(LB94)交换相关势的结果,这些结果表明了几种稀有气体,双原子和水分子的多极极化率和弥散系数。 。 LB94势因其正确的库仑渐近行为而显然表现最佳,其结果接近于多体摄动理论(MBPT)所获得的结果。对于各向同性特性,LDA和BP结果在系统上过高。对于较高的色散系数,这将逐渐变得更糟。然而,相对各向异性的结果对于所有三个电势而言都是令人满意的。 (C)1997美国物理研究所。 [参考:54]

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