# Spin-Projected Generalized Hartree-Fock as a Polynomial of Particle-Hole Excitations

## TL;DR

This paper demonstrates that spin-projected generalized Hartree-Fock wave functions can be expressed as polynomials of excitation operators, enabling potential integration with coupled cluster methods to better describe both weak and strong electron correlations.

## Contribution

It extends previous work by showing that spin-projected generalized Hartree-Fock wave functions are polynomials of excitation operators, providing a foundation for combined methods with coupled cluster theory.

## Key findings

- Wave functions are expressible as low-order excitation polynomials.
- Preliminary applications to the Hubbard model show promise.
- Method could improve accuracy across correlation regimes.

## Abstract

The past several years have seen renewed interest in the use of symmetry-projected Hartree-Fock for the description of strong correlations. Unfortunately, these symmetry-projected mean-field methods do not adequately account for dynamic correlation. Presumably, this shortcoming could be addressed if one could combine symmetry-projected Hartree-Fock with a many-body method such as coupled cluster theory, but this is by no means straightforward because the two techniques are formulated in very different ways. However, we have recently shown that the singlet $S^2$-projected unrestricted Hartree-Fock wave function can in fact be written in a coupled cluster-like wave function: that is, the spin-projected unrestricted Hartree-Fock wave function can be written as a polynomial of a double-excitation operator acting on some closed-shell reference determinant. Here, we extend this result and show that the spin-projected generalized Hartree-Fock wave function (which has both $S^2$ and $S_z$ projection) is likewise a polynomial of low-order excitation operators acting on a closed-shell determinant, and provide a closed-form expression for the resulting polynomial coefficients. We include a few preliminary applications of the combination of this spin-projected Hartree-Fock and coupled cluster theory to the Hubbard Hamiltonian, and comment on generalizations of the methodology. Results here are not for production level, but a similarity transformed theory that combines the two offers the promise of being accurate for both weak and strong correlation, and particularly may offer significant improvements in the intermediate correlation regime where neither projected Hartree-Fock nor coupled cluster is particularly accurate.