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The variational two-electron reduced-density-matrix method for extended systems.

机译:扩展系统的变分二电子密度降低矩阵方法。

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摘要

In this thesis we develop the variational two-electron reduced-density-matrix method for extended systems. Extended systems are represented in two ways: i) lattice models describing the dominant valence electronic structure with periodic boundaries to account for their extended nature and ii) a crystalline-orbital basis built from atomic orbitals using the generalization of molecular orbital theory to polymers.;The first part of this thesis (Ch. 3--4) examines the performance of the variational 2-RDM method on lattice systems with tunable electron correlation. The first of these systems is the classic Hubbard model with linear and ladder lattice topologies. Because electron correlation functions, such as charge- and spin-ordering, are linear functions of the 2-RDM, the difference in electronic structure between one- and quasi-one-dimensional systems is accurately characterized. The second model contains only two-body interactions and is unique among typical spin models in that it does not have a mean-field reference wave function. The ground state wave functions from all Hamiltonians in the model have the same 1-electron reduced density matrix; consequently, one-electron theories are largely inapplicable. The superconducting eta-pairing ground states make the model a unique tool for demonstrating the necessary N-representability in highly correlated environments.;The second part of this thesis (Ch. 5--6) develops a formalism for modeling materials by solving the full Schrodinger equation. Crystalline-orbital Hartree-Fock provides a set of orbitals and integral tensors for the variational 2-RDM method. We demonstrate that time-reversal symmetry, which is implicitly included in position space electronic structure calculations, must be explicitly included as an N-representability constraint on the 2-RDM when using a momentum space basis. The necessity of these equality constraints is demonstrated by the accurate recovery of the binding energy of two polymers and the symmetry of their natural orbital occupations.
机译:本文针对扩展系统开发了变分双电子降密度矩阵方法。扩展系统以两种方式表示:i)描述具有周期性边界的主导价电子结构的晶格模型,以解释其扩展性质; ii)使用分子轨道理论推广到聚合物由原子轨道构建的晶体轨道基础;本文的第一部分(第3--4章)研究了变分2-RDM方法在具有可调电子相关性的晶格系统上的性能。这些系统中的第一个是具有线性和梯形晶格拓扑的经典Hubbard模型。由于电子相关函数(例如电荷排序和自旋排序)是2-RDM的线性函数,因此一维和准一维系统之间电子结构的差异得以准确表征。第二个模型仅包含两体相互作用,并且在典型的自旋模型中是唯一的,因为它没有均值参考波函数。模型中所有哈密顿量的基态波函数都具有相同的1电子降密度矩阵。因此,单电子理论在很大程度上是不适用的。超导η-配对基态使该模型成为证明在高度相关的环境中必要的N表示性的独特工具。本论文的第二部分(第5--6章)通过求解材料的全过程为材料建模提供了形式主义。薛定inger方程。晶体轨道Hartree-Fock为变分2-RDM方法提供了一组轨道和积分张量。我们证明,使用动量空间基础时,位置空间电子结构计算中隐式包含的时间反转对称性必须作为2-RDM上的N可表示性约束明确包含在内。这些相等性约束的必要性通过两种聚合物的结合能的准确恢复和其自然轨道占据的对称性得到证明。

著录项

  • 作者

    Rubin, Nicholas C.;

  • 作者单位

    The University of Chicago.;

  • 授予单位 The University of Chicago.;
  • 学科 Physical chemistry.;Condensed matter physics.
  • 学位 Ph.D.
  • 年度 2016
  • 页码 113 p.
  • 总页数 113
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 宗教;
  • 关键词

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