Magnetization-induced reordering of ground states phase diagram in a two-component Bose-Hubbard model
arXiv:2508.06442 · doi:10.1103/z78x-bd1k
Abstract
We investigate the influence of non-zero magnetization on the ground-state phase diagram of the two-component Bose-Hubbard model. Employing a mean-field theoretical framework, both analytically and numerically, we demonstrate that positions and sizes of specific phases on the diagram are magnetization dependent. In particular, non-zero magnetization introduces different Mott insulator phase boundaries for each of the two components. This effect leads to the emergence of a hybrid phase characterized by the coexistence of superfluid in one of the components and Mott insulator in the another one. Our findings highlight the important role of a conserved quantities, which is magnetization here, in reshaping the phase landscape, significantly influencing the stability and emergence of distinct quantum phases.
9 pages, 4 figures
References in corpus (10)
- Probing many-body dynamics on a 51-atom quantum simulator
- Non-standard Hubbard models in optical lattices: a review
- Detecting Chiral Edge States in the Hofstadter Optical Lattice
- Density wave and supersolid phases of correlated bosons in an optical lattice
- Supersolidity in ultra-cold dipolar gases
- Quantum Gutzwiller approach for the two-component Bose-Hubbard model
- Preparation of the spin-Mott state: a spinful Mott insulator of repulsively bound pairs
- Formation of stripes in a mixed-dimensional cold-atom Fermi-Hubbard system
- Observation of counterflow superfluidity in a two-component Mott insulator
- Hubbard physics with Rydberg atoms: using a quantum spin simulator to simulate strong fermionic correlations