Exotic quantum liquids in Bose-Hubbard models with spatially-modulated
symmetries
- URL: http://arxiv.org/abs/2307.08761v2
- Date: Thu, 11 Jan 2024 05:20:02 GMT
- Title: Exotic quantum liquids in Bose-Hubbard models with spatially-modulated
symmetries
- Authors: Pablo Sala, Yizhi You, Johannes Hauschild, Olexei Motrunich
- Abstract summary: We investigate the effect that spatially modulated continuous conserved quantities can have on quantum ground states.
We show that such systems feature a non-trivial Hilbert space fragmentation for momenta incommensurate with the lattice.
We conjecture that a Berezinskii-Kosterlitz-Thouless-type transition is driven by the unbinding of vortices along the temporal direction.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: We investigate the effect that spatially modulated continuous conserved
quantities can have on quantum ground states. We do so by introducing a family
of one-dimensional local quantum rotor and bosonic models which conserve finite
Fourier momenta of the particle number, but not the particle number itself.
These correspond to generalizations of the standard Bose-Hubbard model (BHM),
and relate to the physics of Bose surfaces. First, we show that while having an
infinite-dimensional local Hilbert space, such systems feature a non-trivial
Hilbert space fragmentation for momenta incommensurate with the lattice. This
is linked to the nature of the conserved quantities having a dense spectrum and
provides the first such example. We then characterize the zero-temperature
phase diagram for both commensurate and incommensurate momenta. In both cases,
analytical and numerical calculations predict a phase transition between a
gapped (Mott insulating) and quasi-long range order phase; the latter is
characterized by a two-species Luttinger liquid in the infrared, but dressed by
oscillatory contributions when computing microscopic expectation values.
Following a rigorous Villain formulation of the corresponding rotor model, we
derive a dual description, from where we estimate the robustness of this phase
using renormalization group arguments, where the driving perturbation has
ultra-local correlations in space but power law correlations in time. We
support this conclusion using an equivalent representation of the system as a
two-dimensional vortex gas with modulated Coulomb interactions within a fixed
symmetry sector. We conjecture that a Berezinskii-Kosterlitz-Thouless-type
transition is driven by the unbinding of vortices along the temporal direction.
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