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PreprintCC BY 4.0arXiv

Finite-volume and thermodynamic-limit lower bounds for the coherently driven Bose--Hubbard model via the Lieb--Yamazaki method

Abstract

We derive rigorous lower bounds on the ground-state energy of the coherently driven Bose--Hubbard model using a Lieb--Yamazaki positive-operator decomposition. The resulting quadratic bounding Hamiltonian is diagonalized by displacement and Bogoliubov transformations, yielding explicit stability conditions and finite-volume bounds in arbitrary dimension. We establish the thermodynamic-limit energy density and characterize the excitation spectrum of the bounding Hamiltonian. We also derive its Gaussian-state observables, including filling, number fluctuations, and second-order correlations, and identify regimes of antibunching and sub-Poissonian statistics. Numerical calculations assess the tightness of the bounds across representative parameter regimes.

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BibTeX
@misc{janowicz2026finitevolume,
  title = {{Finite-volume and thermodynamic-limit lower bounds for the coherently driven Bose--Hubbard model via the Lieb--Yamazaki method}},
  author = {Maciej Janowicz and Joanna Kaleta and Filip Krzyżewski and Andrzej Zembrzuski},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.38464},
  eprint = {2610.38464},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.38464},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Finite-volume and thermodynamic-limit lower bounds for the coherently driven Bose--Hubbard model via the Lieb--Yamazaki method
AU  - Maciej Janowicz
AU  - Joanna Kaleta
AU  - Filip Krzyżewski
AU  - Andrzej Zembrzuski
PY  - 2026
DA  - 2026/10/28
PB  - arXiv
DO  - 10.48550/arxiv.2610.38464
UR  - https://arxiv.org/abs/2610.38464
AB  - We derive rigorous lower bounds on the ground-state energy of the coherently driven Bose--Hubbard model using a Lieb--Yamazaki positive-operator decomposition. The resulting quadratic bounding Hamiltonian is diagonalized by displacement and Bogoliubov transformations, yielding explicit stability conditions and finite-volume bounds in arbitrary dimension. We establish the thermodynamic-limit energy density and characterize the excitation spectrum of the bounding Hamiltonian. We also derive its Gaussian-state observables, including filling, number fluctuations, and second-order correlations, and identify regimes of antibunching and sub-Poissonian statistics. Numerical calculations assess the tightness of the bounds across representative parameter regimes.
ER  -