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Sparse non-orthogonal wave function expansions from the extension of the generalized Pauli constraints to the two-electron reduced density matrix

机译:稀疏的非正交波函数扩展从广义的Pauli延伸到两电子降低密度矩阵

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摘要

Generalized Pauli constraints (GPCs) impose constraints in the form of inequalities on the natural orbital occupation numbers of the one electron reduced density matrix (1-RDM), defining the set of pure N-representable 1-RDMs, or 1-RDMs that can be derived from an N-electron wave function. Saturation of these constraints is termed "pinning" and implies a significant simplification of the N-electron wave function as the number of Slater determinants required to fully describe the system is reduced. Recent research has shown pinning to occur for the ground states of atoms and molecules with N = 3 and r = 6, where N is the number of electrons and r is the number of spin orbitals. For N = 4 and r = 8, however, pinning occurs not to the GPCs but rather to inequalities defining the pure N-representable two-electron reduced density matrices (2-RDMs). Using these more general inequalities, we derive a wave function ansatz for a system with four electrons in eight spin orbitals. We apply the ansatz to the isoelectronic series of the carbon atom and the dissociation of linear H-4 where the correlation energies are recovered to fractions of a kcal/mol. These results provide a foundation for further developments in wave function and RDM theories based on "pinned" solutions, and elucidate a fundamental physical basis for the emergence of non-orthogonal bases in electronic systems of N >= 4.
机译:广义的Pauli约束(GPC)以一种电子降低密度矩阵(1-RDM)的天然轨道占据数量的不等式的形式施加约束,定义了一组纯N-可代表1-RDMS,或1-RDM来自N-电子波函数。这些约束的饱和被称为“钉扎”,并且暗示N型电子波函数的显着简化,因为需要完全描述系统所需的替换器的数量。最近的研究表明,用n = 3和r = 6的原子和分子发生钉扎,其中n是电子的数量,R是旋转轨道的数量。然而,对于n = 4和r = 8,钉扎出不到GPC,而是不平等地定义纯N-Implayable的二电子减小密度矩阵(2-RDMS)。使用这些更普遍的不等式,我们为八个旋转轨道有四个电子的系统导出了一个系统的波函​​数Ansatz。我们将Ansatz应用于碳原子的异形系列和线性H-4的解离,其中相关能量被回收到Kcal / mol的级分。这些结果为基于“固定”解决方案的波浪功能和RDM理论的进一步发展提供了基础,并阐明了N> = 4的电子系统中非正交碱基出现的基本物理基础。

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