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Journal ArticleDOI

n‐Representability Problem for Reduced Density Matrices

Hans Kummer
- 01 Oct 1967 - 
- Vol. 8, Iss: 10, pp 2063-2081
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TLDR
In this article, it was shown that a density operator Dp belongs to Tnp¯ (the bar indicates the closure with respect to a certain topology) if and only if Tr (DpBp) ≥ 0 for all bounded self-adjoint p-particle operators Bp, such that their n−expansion (pn)ΓpnBp≡ ∑ i1<…<ipBp(i1…ip) is a positive operator in n-particles space.
Abstract
In this paper we prove some theorems about the n‐representability problem for reduced density operators. The first theorem (Theorem 6) sharpens a theorem proved by Garrod and Percus. Let Tnp be the set of all n‐representable p‐density operators. Then a density operator Dp belongs to Tnp¯ (the bar indicates the closure with respect to a certain topology) if and only if Tr (DpBp) ≥ 0 for all bounded self‐adjoint p‐particle operators Bp, such that their n‐expansion (pn)ΓpnBp≡ ∑ i1<…<ipBp(i1…ip) is a positive operator in n‐particle space. Moreover, it is shown that Tnp¯ is the closed convex hull of the exposed points of Tnp of finite one‐rank (Theorem 9). A more practical version of this theorem may be formulated in the following manner (cf. Theorem 8).Consider the set γp of subspaces of the n‐particle space, occurring as an eigenspace to the deepest eigenvalue of a bounded n‐particle operator which is the n expansion of some p‐particle operator. Choose from every element of γp one (and only one) vector (func...

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Journal ArticleDOI

Variational calculations of fermion second-order reduced density matrices by semidefinite programming algorithm

TL;DR: The ground-state fermion second-order reduced density matrix (2-RDM) is determined variationally using itself as a basic variable using the positive semidefiniteness conditions, P, Q, and G conditions that are described in terms of the 2-R DM.
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Structure of Fermionic Density Matrices: Complete N-Representability Conditions

TL;DR: A hierarchy of constraints built upon the bipolar theorem and tensor decompositions of model Hamiltonians is derived, which are amenable to polynomial-time computations of strongly correlated systems.
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Approximating q -order reduced density matrices in terms of the lower-order ones. I. General relations

TL;DR: A general and closed-form relation is obtained here, in this equation the part involving RDM's has the same structure as that involving hole reduced density matrices.
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The variational approach to the two−body density matrix

TL;DR: In this article, a variational method for the two-body density matrix is developed for practical calculations of the properties of many-fermion systems with two−body interactions, in which the energy E = JHijkl ρijkl is minimized using the two−Body density matrix elements ρjkl = 〈ψ‖a+ja+iakal‖ψ〉 as variational parameters.
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The Electronic Ground State Energy Problem: a New Reduced Density Matrix Approach

TL;DR: In this paper, the ground-state energy of a two-electron reduced Hamiltonian on the dual cone of a dual cone has been derived using a duality argument based on the second-order reduced density matrix.
References
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Mathematical Foundations of Quantum Mechanics

TL;DR: The Mathematical Foundations of Quantum Mechanics as discussed by the authors is a seminal work in theoretical physics that introduced the theory of Hermitean operators and Hilbert spaces and provided a mathematical framework for quantum mechanics.

Mathematical Foundations of Quantum Mechanics

TL;DR: The Mathematical Foundations of Quantum Mechanics as discussed by the authors is a seminal work in theoretical physics that introduced the theory of Hermitean operators and Hilbert spaces and provided a mathematical framework for quantum mechanics.
Journal ArticleDOI

Structure of Fermion Density Matrices

TL;DR: In this paper, a new approach is presented to the many-particle problem in quantum mechanics by proposing a method of finding natural orbitals and natural geminals of a system without prior knowledge of the wave function.
Journal ArticleDOI

Reduction of the N‐Particle Variational Problem

TL;DR: In this paper, a variational method is presented which is applicable to N-particle boson or fermion systems with two-body interactions, and it is proven that if Γ(1, 2 | 1′, 2′) and γ(1| 1′) are the twoparticle and oneparticle density matrices of an N−particle system [normalized by tr Γ = N(N − 1) and trγ = N] then the associated operator: G( 1, 2|| 1′,2
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