Symmetry-projected cluster mean-field theory applied to spin systems
arXiv:2304.12822 · doi:10.1063/5.0155765
Abstract
We introduce spin-projection based on cluster mean-field theory and apply it to the ground state of strongly-correlated spin systems. In cluster mean-field, the ground state wavefunction is written as a factorized tensor product of optimized cluster states. In previous work, we have focused on unrestricted cluster mean-field, where each cluster is symmetry adapted. We here remove this restriction by introducing a generalized cluster mean-field (GcMF) theory, where each cluster is allowed to access all sectors, breaking symmetry. In addition, a projection scheme is used to restore global , which gives rise to spin-projected generalized cluster mean-field (SGcMF). Both of these extensions contribute to accounting for inter-cluster correlations. We benchmark these methods on the 1D, quasi-2D, and 2D and Heisenberg models. Our results indicate that the new methods (GcMF and SGcMF) provide a qualitative and semi-quantitative description of the Heisenberg lattices in the regimes considered, suggesting them as useful references for further inter-cluster correlations, which are discussed in this work.
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