Phase Dilemma in Natural Orbital Functional Theory from the N-representability Perspective

TL;DR

This paper investigates the phase dilemma in natural orbital functional theory from the N-representability perspective, showing its occurrence in both top-down and bottom-up methods and demonstrating its importance in accurately modeling strongly correlated systems.

Contribution

It reveals the presence of the phase dilemma in bottom-up N-representability approaches and proposes specific sign choices to improve modeling of strongly correlated systems.

Findings

The phase dilemma appears in bottom-up methods as well as top-down.

Correct sign choices are crucial for modeling strong electron correlation.

PNOF7 functional with specific phase choices matches exact results for model systems.

Abstract

Any rigorous approach to first-order reduced density (1RDM) matrix functional theory faces the phase dilemma, that is, having to deal with a large number of possible combinations of signs in terms of the electron-electron interaction energy. This problem was discovered by reducing a ground-state energy generated from an approximate N-particle wavefunction into a functional of the 1RDM, known as the top-down method. Here, we show that the phase dilemma also appears in the bottom-up method, in which the functional E[1RDM] is generated by progressive inclusion of N-representability conditions on the reconstructed two-particle reduced density matrix. It is shown that an adequate choice of signs is essential to accurately describe model systems with strong non-dynamic (static) electron correlation, specifically, the one-dimensional Hubbard model with periodic boundary conditions and hydrogen rings. For the latter, the Piris natural orbital functional 7 (PNOF7), with phases equal to -1 for the inter-pair energy terms containing the exchange-time-inversion integrals, agrees with exact diagonalization results.