4 research outputs found
Localization and spectrum of quasiparticles in a disordered fermionic Dicke model
We study a fermionic two-band model with the interband transition resonantly
coupled to a cavity. This model was recently proposed to explain
cavity-enhanced charge transport, but a thorough characterization of the closed
system, in particular localization of various excitations, is lacking. In this
work, using exact diagonalization, we characterize the system by its spectrum
under various filling factors and variable disorder. As in the Dicke model, the
effective light-matter coupling scales with the square root of the system size.
However, there is an additional factor that decreases with increasing doping
density. The transition from the weak-coupling regime to the strong-coupling
regime occurs when the effective light-matter coupling is larger than the
electronic bandwidth. Here, the formation of exciton-polaritons is accompanied
by the formation of bound excitons. Photon spectral functions exhibit
significant weights on the in-gap states between the polaritons, even without
disorder. Finally, while the localization of electron-hole excitations in a
disordered system is lifted by strong coupling, the same is not true for free
charges, which remain localized at strong and even ultrastrong coupling. Based
on this finding, we discuss scenarios for charge transport
Interaction-driven dynamical quantum phase transitions in a strongly correlated bosonic system
We study dynamical quantum phase transitions (DQPTs) in the extended
Bose-Hubbard model after a sudden quench of the nearest-neighbor interaction
strength. Using the time-dependent density matrix renormalization group, we
demonstrate that interaction-driven DQPTs can appear after quenches between two
topologically trivial insulating phases -- a phenomenon that has so far only
been studied between gapped and gapless phases. These DQPTs occur when the
interaction strength crosses a certain threshold value that does not coincide
with the equilibrium phase boundaries, which is in contrast to quenches that
involve a change of topology. In order to elucidate the nonequilibrium
excitations during the time evolution, we define a new set of string and parity
order parameters. We find a close connection between DQPTs and these newly
defined order parameters for both types of quenches. In the interaction-driven
case, the order parameter exhibits a singularity at the time of the DQPT only
when the quench parameter is close to the threshold value. Finally, the
timescales of DQPTs are scrutinized and different kinds of power laws are
revealed for the topological and interaction-driven cases.Comment: 6 pages, 4 figures, and supplemental materia