Competing order in two-band Bose-Hubbard chains with extended-range interactions

Motivated by the recent progress in realizing and controlling extended Bose-Hubbard systems using excitonic or atomic devices, the present Letter theoretically investigates the case of a two-band Bose-Hubbard chain with nearest-neighbor interactions. Specifically, this study concentrates on the scen...

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Detalles Bibliográficos
Autores: Watanabe, Yuma, Bhattacharya, Utso, Chhajlany, Ravindra W., Argüello Luengo, Javier|||0000-0001-5627-8907, Lewenstein, Maciej, Grass, Tobias Daniel
Tipo de recurso: artículo
Fecha de publicación:2024
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/406539
Acceso en línea:https://hdl.handle.net/2117/406539
https://dx.doi.org/10.1103/PhysRevB.109.L100507
Access Level:acceso abierto
Palabra clave:Bosons
Quantum theory
Quàntums, Teoria dels
Àrees temàtiques de la UPC::Física::Mecànica quàntica
Descripción
Sumario:Motivated by the recent progress in realizing and controlling extended Bose-Hubbard systems using excitonic or atomic devices, the present Letter theoretically investigates the case of a two-band Bose-Hubbard chain with nearest-neighbor interactions. Specifically, this study concentrates on the scenario where, due to the interactions, one band supports a density-wave phase, i.e., a correlated insulating phase with spontaneous breaking of translational symmetry in the lattice, while the other band supports superfluid behavior. Using the density matrix renormalization group method, we show that supersolid order can emerge from such a combination, that is, an elusive quantum state that combines crystalline order with long-range phase coherence. Depending on the f illing of the bands and the interband interaction strength, the supersolid phase competes with phase-separation, superfluid order, or Mott insulating density-wave order. As a possible setup to observe supersolidity, we propose the combination of a lower band supporting density-wave order and a thermally excited band that supports superfluidity due to weaker lattice confinement.