216 research outputs found
Extremely long-lived universal resonant Bose gases
Quantum simulations based on near-resonance Bose gases are limited by their
short lifetimes due to severe atom losses. In addition to this, the recently
predicted thermodynamical instability adds another constraint on accessing the
resonant Bose gases. In this Letter, we offer a potential solution by proposing
long-lived resonant Bose gases in both two and three dimensions, where the
conventional few-body losses are strongly suppressed. We show that the
thermodynamical properties as well as the lifetimes of these strongly
interacting systems are universal, and independent of short-range physics.Comment: 5 page
Transport in p-wave interacting Fermi gases
The scattering properties of spin-polarized Fermi gases are dominated by
p-wave interactions. Besides their inherent angular dependence, these
interactions differ from their s-wave counterparts as they also require the
presence of a finite effective range in order to understand the low-energy
properties of the system. In this article we examine how the shear viscosity
and thermal conductivity of a three-dimensional spin-polarized Fermi gas in the
normal phase depend on the effective range and the scattering volume in both
the weakly and strongly interacting limits. We show that although the shear
viscosity and thermal conductivity both explicitly depend on the effective
range near resonance, the Prandtl number which parametrizes the ratio of
momentum to thermal diffusivity does not have an explicit interaction
dependence both at resonance and for weak interactions in the low-energy limit.
In contrast to s-wave systems, p-wave scattering exhibits an additional
resonance at weak attraction from a quasi-bound state at positive energies,
which leads to a pronounced dip in the shear viscosity at specific
temperatures.Comment: 12 pages, 7 figures; published versio
Far-Away-From-Equilibrium Quantum Critical Conformal Dynamics: Reversibility, Thermalization, and Hydrodynamics
Generic far-away-from-equilibrium many-body dynamics usually involve entropy
production, and hence are thermodynamically irreversible. Near quantum critical
points, an emergent conformal symmetry can impose strong constraints on entropy
production rates, and in some cases completely forbid entropy production, which
usually occurs for systems that deviate from quantum critical points. In this
letter, we illustrate how the vanishing entropy production near a quantum
critical point, and at finite temperatures, results in reversible
far-away-from-equilibrium dynamics that are otherwise irreversible. Our
analysis directly relates the thermalization time scale to the hydrodynamic
viscosity near quantum critical points with dynamical critical exponent .
Both controllable reversible and irreversible dynamics can be potentially
studied in cold gas experiments.Comment: 5 pages, 4 figure
Emergent Infrared Conformal Dynamics in Strongly Interacting Quantum Gases
Conformal dynamics can appear in quantum gases when the interactions are fine
tuned to be scale symmetric. One well-known example of such a system is a
three-dimensional Fermi gas at a Feshbach resonance. In this letter, we
illustrate how conformal dynamics can also emerge in the infrared limit in
one-dimensional harmonically trapped Fermi gases, even though the system may
not have exactly scale symmetric interactions. The conformal dynamics are
induced by strong renormalization effects due to the nearby infrared stable
scale invariant interaction. When the system approaches the infrared limit, or
when the external harmonic trapping frequency , the
dynamics are characterized by a unique vanishingly small dissipation rate,
, rather than a constant as in generic interacting
systems. We also examine the work done in a two-quench protocol, , and the
average power . In one dimension, the average power, , becomes vanishingly small in the infrared limit, a signature
of emergent conformal dynamics.Comment: 6 pages, 3 figure
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