338 research outputs found
Disordered flat bands on the kagome lattice
We study two models of correlated bond- and site-disorder on the kagome
lattice considering both translationally invariant and completely disordered
systems. The models are shown to exhibit a perfectly flat ground state band in
the presence of disorder for which we provide exact analytic solutions. Whereas
in one model the flat band remains gapped and touches the dispersive band, the
other model has a finite gap, demonstrating that the band touching is not
protected by topology alone. Our model also displays fully saturated
ferromagnetic groundstates in the presence of repulsive interactions, an
example of disordered flat band ferromagnetism.Comment: 7+3 pages, 4+2 figures, accepted versio
Temperature dependence of butterfly effect in a classical many-body system
We study the chaotic dynamics in a classical many-body system of interacting
spins on the kagome lattice. We characterise many-body chaos via the butterfly
effect as captured by an appropriate out-of-time-ordered correlator. Due to the
emergence of a spin liquid phase, the chaotic dynamics extends all the way to
zero temperature. We thus determine the full temperature dependence of two
complementary aspects of the butterfly effect: the Lyapunov exponent, ,
and the butterfly speed, , and study their interrelations with usual
measures of spin dynamics such as the spin-diffusion constant, and
spin-autocorrelation time, . We find that they all exhibit power law
behaviour at low temperature, consistent with scaling of the form and . The vanishing of is
parametrically slower than that of the corresponding quantum bound, , raising interesting questions regarding the semi-classical limit of such
spin systems.Comment: 6+4 pages, 4+8 figures, ancillary files include videos of the
dynamic
Risk-based management of chemicals and products in a circular economy at a global scale- Impacts of the FP7 funded project RISKCYCLE
Synthetic dimensions in the strong-coupling limit: Supersolids and pair superfluids
We study the many-body phases of bosonic atoms with internal states
confined to a 1D optical lattice under the influence of a synthetic magnetic
field and strong repulsive interactions. The internal states of the atoms
are coupled via Raman transitions creating the synthetic magnetic field in the
space of internal spin states corresponding to recent experimental
realisations. We focus on the case of strong \mbox{SU}(N) invariant local
density-density interactions in which each site of the 1D lattice is at most
singly occupied, and strong Raman coupling, in distinction to previous work
which has focused on the weak Raman coupling case. This allows us to keep only
a single state per site and derive a low energy effective spin model. The
effective model contains first-order nearest neighbour tunnelling terms, and
second-order nearest neighbour interactions and correlated next-nearest
neighbour tunnelling terms. By adjusting the flux one can tune the
relative importance of first-order and second-order terms in the effective
Hamiltonian. In particular, first-order terms can be set to zero, realising a
novel model with dominant second-order terms. We show that the resulting
competition between density-dependent tunnelling and repulsive density-density
interaction leads to an interesting phase diagram including a phase with
long-ranged pair-superfluid correlations. The method can be straightforwardly
extended to higher dimensions and lattices of arbitrary geometry including
geometrically frustrated lattices where the interplay of frustration,
interactions and kinetic terms is expected to lead to even richer physics.Engineering and Physical Sciences Research Council (Grant ID: EP/K030094/1)This is the author accepted manuscript. The final version is available from the American Physical Society via http://dx.doi.org/10.1103/PhysRevA.94.02363
Scattering theory for Floquet-Bloch states
Motivated by recent experimental implementations of artificial gauge fields
for gases of cold atoms, we study the scattering properties of particles that
are subjected to time-periodic Hamiltonians. Making use of Floquet theory, we
focus on translationally invariant situations in which the single-particle
dynamics can be described in terms of spatially extended Floquet-Bloch waves.
We develop a general formalism for the scattering of these Floquet-Bloch waves.
An important role is played by the conservation of Floquet quasi-energy, which
is defined only up to the addition of integer multiples of for a
Hamiltonian with period . We discuss the consequences of this
for the interpretation of "elastic" and "inelastic" scattering in cases of
physical interest. We illustrate our general results with applications to: the
scattering of a single particle in a Floquet-Bloch state from a static
potential; and, the scattering of two particles in Floquet-Bloch states through
their interparticle interaction. We analyse examples of these scattering
processes that are closely related to the schemes used to general artifical
gauge fields in cold-atom experiments, through optical dressing of internal
states, or through time-periodic modulations of tight-binding lattices. We show
that the effects of scattering cannot, in general, be understood by an
effective time-independent Hamiltonian, even in the limit
of rapid modulation. We discuss the relative sizes of the elastic scattering
(required to stablize many-body phases) and of the inelastic scattering
(leading to deleterious heating effects). In particular, we describe how
inelastic processes that can cause significant heating in current experimental
set-up can be switched off by additional confinement of transverse motion.This work was supported by EPSRC Grant No. EP/K030094/1.This is the accepted manuscript of a paper published in Physical Review A (Bilitewski T, Cooper NR, Physical Review A 2015, 91, 033601, doi:10.1103/PhysRevA.91.033601). The final version is available at http://dx.doi.org/10.1103/PhysRevA.91.03360
Population dynamics in a Floquet realization of the Harper-Hofstadter Hamiltonian
We study the recent Floquet-realisation of the Harper-Hofstadter model in a
gas of cold bosonic atoms. We study in detail the scattering processes in this
system in the weakly interacting regime due to the interplay of particle
interactions and the explicit time dependence of the Floquet states that lead
to band transitions and heating. We focus on the experimentally used parameters
and explicitly model the transverse confining direction. Based on transition
rates computed within the Floquet-Fermi golden rule we obtain band population
dynamics which are in agreement with the dynamics observed in experiment.
Finally, we discuss whether and how photon-assisted collisions that may be the
source heating and band population dynamics might be suppressed in the
experimental setup by appropriate design of the transverse confining potential.
The suppression of such processes will become increasingly important as the
experiments progress into simulating strongly interacting systems in the
presence of artificial gauge fields.This work was supported by EPSRC Grant No EP/K030094/1.This is the accepted manuscript. The final version is available at http://journals.aps.org/pra/abstract/10.1103/PhysRevA.91.063611
Radial flows and angular momentum conservation in galactic chemical evolution
We study the effects of radial flows on Galactic chemical evolution. A simple analytic scheme is developed prescribing the coupling of infall from the intergalactic medium and radial flows within the disc based on angular momentum conservation.Physic
Exotic superconductivity through bosons in a dynamical cluster approximation
We study the instabilities towards (exotic) superconductivity of mixtures of spin-1/2 fermions coupled to scalar bosons on a two-dimensional square lattice with the Dynamical-Cluster-Approximation (DCA) using a numerically exact continuous-time Monte-Carlo solver. The Bogoliubov bosons provide an effective phononic bath for the fermions and induce a non-local retarded interaction between the fermions, which can lead to (exotic) superconductivity. Because of the sign problem the biggest clusters we can study are limited to 2 X 2 in size, but this nevertheless allows us to study the pairing instablilities, and their possible divergence, in the s- and d -wave channels as well as the competition with antiferromagnetic uctuations. At fermionic half-filling we find that d-wave is stable when the mediated interaction by the bosons is of the same order as the bare fermionic repulsion. Its critical temperature can be made as high as the maximum one for s-wave, which opens perspectives for its detection in a cold atom experiment.Physic
Disordered flat bands on the kagome lattice
We study two models of correlated bond- and site-disorder on the kagome lattice considering both translationally invariant and completely disordered systems. The models are shown to exhibit a perfectly at ground state band in the presence of disorder for which we provide exact analytic solutions. Whereas in one model the at band remains gapped and touches the dispersive band, the other model has a finite gap, demonstrating that the band touching is not protected by topology alone. Our model also displays fully saturated ferromagnetic groundstates in the presence of repulsive interactions, an example of disordered at band ferromagnetism.Physic
- …