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Atomic spectral methods for molecular electronic structure calculations

机译:用于分子电子结构计算的原子光谱方法

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Theoretical methods are reported for ab initio calculations of the adiabatic (Born-Oppenheimer) electronic wave functions and potential energy surfaces of molecules and other atomic aggregates. An outer product of complete sets of atomic eigenstates familiar from perturbation-theoretical treatments of long-range interactions is employed as a representational basis without prior enforcement of aggregate wave function antisymmetry. The nature and attributes of this atomic spectral-product basis are indicated, completeness proofs for representation of antisymmetric states provided, convergence of Schrodinger eigenstates in the basis established, and strategies for computational implemention of the theory described. A diabaticlike Hamiltonian matrix representative is obtained, which is additive in atomic-energy and pairwise-atomic interaction-energy matrices, providing a basis for molecular calculations in terms of the (Coulombic) interactions of the atomic constituents. The spectral-product basis is shown to contain the totally antisymmetric irreducible representation of the symmetric group of aggregate electron coordinate permutations once and only once, but to also span other (non-Pauli) symmetric group representations known to contain unphysical discrete states and associated continua in which the physically significant Schrodinger eigenstates are generally embedded. These unphysical representations are avoided by isolating the physical block of the Hamiltonian matrix with a unitary transformation obtained from the metric matrix of the explicitly antisymmetrized spectral-product basis. A formal proof of convergence is given in the limit of spectral closure to wave functions and energy surfaces obtained employing conventional prior antisymmetrization, but determined without repeated calculations of Hamiltonian matrix elements as integrals over explicitly antisymmetric aggregate basis states. Computational implementations of the theory employ efficient recursive methods which avoid explicit construction the metric matrix and do not require storage of the full Hamiltonian matrix to isolate the antisymmetric subspace of the spectral-product representation. Calculations of the lowest-lying singlet and triplet electronic states of the covalent electron pair bond (H-2) illustrate the various theorems devised and demonstrate the degree of convergence achieved to values obtained employing conventional prior antisymmetrization. Concluding remarks place the atomic spectral-product development in the context of currently employed approaches for ab initio construction of adiabatic electronic eigenfunctions and potential energy surfaces, provide comparisons with earlier related approaches, and indicate prospects for more general applications of the method. (C) 2004 American Institute of Physics.
机译:报道了从理论上计算绝热(Born-Oppenheimer)电子波函数以及分子和其他原子团聚体的势能面的理论方法。可以采用长期相互作用的扰动-理论处理所熟悉的原子本征态的完整集合的外部产物作为表示基础,而无需事先执行聚集波函数反对称性。指出了该原子光谱乘积基础的性质和属性,提供了表示不对称态的完整性证明,在此基础上建立了薛定inger本征态的收敛性,并描述了该理论的计算实现策略。获得了非绝热状的哈密顿矩阵代表,它是原子能和成对原子相互作用能矩阵的加和,为根据原子成分的(库伦)相互作用提供分子计算的基础。光谱积的基础被证明包含一次和仅一次的总电子坐标排列对称组的完全反对称不可约表示,而且还跨越其他已知包含非物理离散态和相关连续性的对称(非保利)对称组表示通常嵌入具有物理意义的薛定inger本征态。通过用从明确的反对称谱积基础的度量矩阵中获得的unit变换来隔离汉密尔顿矩阵的物理块,可以避免这些非物理表示。在使用常规先验反对称化获得的波函数和能表面的频谱封闭范围内,给出了收敛的形式化证明,但无需对哈密顿矩阵元作为明确反对称聚合基态的积分进行重复计算即可确定。该理论的计算实现采用有效的递归方法,该方法可避免显式构造度量矩阵,并且不需要存储完整的汉密尔顿矩阵即可隔离频谱积表示的反对称子空间。共价电子对键(H-2)的最低单重态和三重态电子态的计算说明了所设计的各种定理,并证明了收敛到采用常规先有抗对称性获得的值的程度。结束语将原子光谱产品的开发置于绝热电子本征函数和势能面从头开始构建的当前采用的方法的背景下,与较早的相关方法进行了比较,并为该方法的更广泛应用指明了前景。 (C)2004年美国物理研究所。

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