Frustrated extended Bose-Hubbard model and deconfined quantum critical points with optical lattices at the anti-magic wavelength
arXiv:2309.03193 · doi:10.1103/PhysRevLett.132.153401
Abstract
The study of geometrically frustrated many-body quantum systems is of central importance to uncover novel quantum mechanical effects. We design a scheme where ultracold bosons trapped in a one-dimensional state-dependent optical lattice are modeled by a frustrated Bose-Hubbard Hamiltonian. A derivation of the Hamiltonian parameters based on Cesium atoms, further show large tunability of contact and nearest-neighbour interactions. For pure contact repulsion, we discover the presence of two phases peculiar to frustrated quantum magnets: the bond-order-wave insulator with broken inversion symmetry and a chiral superfluid. When the nearest-neighbour repulsion becomes sizeable, a further density-wave insulator with broken translational symmetry can appear. We show that the phase transition between the two spontaneously-symmetry-broken phases is continuous, thus representing a one-dimensional deconfined quantum critical point not captured by the Landau-Ginzburg-Wilson symmetry-breaking paradigm. Our results provide a solid ground to unveil the novel quantum physics induced by the interplay of non-local interactions, geometrical frustration, and quantum fluctuations.
7+3 pages, 3+3 figures
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- Interaction dependence of the Hall response for the Bose-Hubbard triangular ladder
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- Exploring Frustration Effects of Strongly Interacting Bosons via the Hall Response
- Blue repulsive potential for dysprosium Bose-Einstein condensates
- Many-body phases from effective geometrical frustration and long-range interactions in a subwavelength lattice
- Non-Landau quantum phase transition in modulated SU(N) Heisenberg spin chains
- Deconfined quantum criticality on a triangular Rydberg array
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