Engineering Quantum Phases of Ultracold Bosons on Lieb Lattice

Abstract The quantum phase transition of the hardcore boson model on a Lieb lattice by quantum Monte Carlo simulations is studied. Considering nearest‐neighbor interchain hopping, the phase diagram of the Bose‐Hubbard model on the Lieb lattice contains solid phases with average density = 2/3, and superfluid phases between solid phases.Two ways of controlling quantum states are discussed: to add an alternating on‐site potential, and to add an alternating hopping amplitude in the X ‐ and Y ‐directions. For the above cases, there exists a new filling state, = 1/3. Adding an alternating on‐site potential to the Hamiltonian, the phase transition from to is sharp and discontinuous, featuring the nature of a first order. Considering a dimerization term, for large V, it is expected that there is a direct transition from the valence‐bond insulator to the CDW as the interaction is strengthened. For the three cases, upper boundary for and lower boundary for are calculated.

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Publication Details

Journal
Fortschritte der Physik
Published
2024-12-21
DOI
https://doi.org/10.1002/prop.202300235
Primary Topic
Cold Atom Physics and Bose-Einstein Condensates
Type
article
Field-Weighted Citation Impact
0.00

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article

Engineering Quantum Phases of Ultracold Bosons on Lieb Lattice

Lin Yang
Fortschritte der Physik
Cold Atom Physics and Bose-Einstein Condensates
article

Engineering Quantum Phases of Ultracold Bosons on Lieb Lattice

Lin Yang
article en

Abstract

Abstract The quantum phase transition of the hardcore boson model on a Lieb lattice by quantum Monte Carlo simulations is studied. Considering nearest‐neighbor interchain hopping, the phase diagram of the Bose‐Hubbard model on the Lieb lattice contains solid phases with average density = 2/3, and superfluid phases between solid phases.Two ways of controlling quantum states are discussed: to add an alternating on‐site potential, and to add an alternating hopping amplitude in the X ‐ and Y ‐directions. For the above cases, there exists a new filling state, = 1/3. Adding an alternating on‐site potential to the Hamiltonian, the phase transition from to is sharp and discontinuous, featuring the nature of a first order. Considering a dimerization term, for large V, it is expected that there is a direct transition from the valence‐bond insulator to the CDW as the interaction is strengthened. For the three cases, upper boundary for and lower boundary for are calculated.

Fortschritte der PhysikVol. 73(1-2)
Beijing Information Science & Technology University (CN)
Beijing Information Science and Technology University
Sustainable cities and communities
Openalex Percentile: Top 78%
Cold Atom Physics and Bose-Einstein Condensates
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