Diagonal N-representability as a method for solving the representability problem

被引:0
|
作者
Mestechkin, M. M. [1 ]
机构
[1] Russian Acad Sci, Semenov Inst Chem Phys, Moscow 119991, Russia
关键词
reduced density matrix; convex programming and variational method; necessary and sufficient linear inequalities for the RDM; classification of density matrix components; REDUCED DENSITY-MATRICES; ELECTRONIC FOCK SPACE; CONSISTENT-FIELD THEORY; LINEAR INEQUALITIES; CONTRACTION OPERATOR; CONSTRUCTION; CONDENSATION; GEOMETRY; SYMMETRY;
D O I
10.1134/S1990793117020087
中图分类号
O64 [物理化学(理论化学)、化学物理学]; O56 [分子物理学、原子物理学];
学科分类号
070203 ; 070304 ; 081704 ; 1406 ;
摘要
The latest results of density matrix theory are summarized in terms of analysis of off-diagonal components. For a given reduced density matrix (RDM) of arbitrary order, the full density matrix is explicitly constructed, from which the RDM is derived by means of the corresponding reduction procedure. Both the matrices satisfy all the necessary conditions, such antisymmetry, normalization, hermiticity, except that the non-negative definiteness of the full DM is not guaranteed. If an RDM satisfies the necessary inequalities with the same number of indices as it has itself, then, as proved here, there is an additive correction to the full DM matrix that turns it into a non-negative definite matrix leading to the same RDM and satisfying the other requirements. This establishes a fundamental fact that these inequalities are sufficient as well, providing the N-representability of the given RDM. The construction is based on the classification, introduced in the article, of the multi-index elements of the RDM and full DM according to their degree of off-diagonality. RDM elements with a predetermined degree of off-diagonality are expressed through full DM elements with the same off-diagonality. This shows that the conventional variational approach to calculating the energy of the system by convex programming methods under the conditions of N-representability (before and even after reaching the minimum energy) generally does not lead to constructing a mixed quantum state composed of solutions to the Schrodinger equation. Therefore, except for the energy, it does not guarantee a correct description of the other properties so long as the conditions of correctness for each particular property are not expressed in terms of the RDM and not incorporated into the specific conditions of N-representability (regardless of the requirement of energy minimization).
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页码:208 / 227
页数:20
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