Lieb's Theorem for Bose Hubbard Models

Fuente: arXiv
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Auteurs principaux: Wei, Zhong-Chao, Zhao, Chong
Format: Preprint
Publié: 2025
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author Wei, Zhong-Chao
Zhao, Chong
author_facet Wei, Zhong-Chao
Zhao, Chong
contents Using a cone-theoretical method, we prove the uniqueness of the ground state for two Bose Hubbard models. The first model is the usual Bose Hubbard model with real hopping coefficients and attractive interactions. The second model is a two-component Bose Hubbard model. Under certain conditions, we show that the ground state in the subspace with particle number $N=2n$($n$ is a positive integer) is unique for both models. For the second model, we show that the ground state has spin along the z-axis $S^{z}=0$. When the hopping coefficients are real, it has zero spin quantum number, i.e., it is a singlet. Our proofs work equally well for any arbitrary finite-size lattice.
format Preprint
id arxiv_https___arxiv_org_abs_2506_10319
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Lieb's Theorem for Bose Hubbard Models
Wei, Zhong-Chao
Zhao, Chong
Mathematical Physics
Strongly Correlated Electrons
Using a cone-theoretical method, we prove the uniqueness of the ground state for two Bose Hubbard models. The first model is the usual Bose Hubbard model with real hopping coefficients and attractive interactions. The second model is a two-component Bose Hubbard model. Under certain conditions, we show that the ground state in the subspace with particle number $N=2n$($n$ is a positive integer) is unique for both models. For the second model, we show that the ground state has spin along the z-axis $S^{z}=0$. When the hopping coefficients are real, it has zero spin quantum number, i.e., it is a singlet. Our proofs work equally well for any arbitrary finite-size lattice.
title Lieb's Theorem for Bose Hubbard Models
topic Mathematical Physics
Strongly Correlated Electrons
url https://arxiv.org/abs/2506.10319