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Journal of Low Temperature Physics

Tunneling critical velocity of a superfluid. [Lifshitz-Kogan theory]

Mitsuhisa Ichiyanagi

Published Jun 1, 1976• 0 citations
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Related papers

Tunneling critical velocity of a superfluid

Masakazu Ichiyanagi

Journal of Low Temperature Physics•Jun 1, 1976•1 citation

Rotating Larkin-Ovchinnikov-Fulde-Ferrell state of the two-dimensional ultracold Fermi superfluid gas: Reentrant behavior of the critical angular velocity

Miodrag L. Kulić, Armen Sedrakian, Dirk H. Rischke

A rotating ultracold $S$-wave superfluid Fermi gas is studied when the mismatch in chemical potentials $\ensuremath{\delta}\ensuremath{\mu}$ (and the population imbalance $\ensuremath{\delta}n$) corresponds to the Larkin-Ovchinnikov-Fulde-Ferrell state in the vicinity of the Lifshitz critical point. It is shown that under these conditions the critical angular velocity ${\ensuremath{\Omega}}_{c2}$ in two-dimensional systems is an oscillating function of temperature and $\ensuremath{\delta}n$ giving rise to reentrant superfluid phases. The reason for this behavior is the population by Cooper pairs of the Landau levels $(n\ensuremath{\ge}1)$ above the lowest one $(n=0)$.

arXiv:0904.4034•Physical Review A•Oct 15, 2009•6 citations

Superfluid Instability and Critical Velocity in Two and Three Dimensions

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Springer series in solid-state sciences•Jan 1, 2013•0 citations

Hydrodynamic equations for a U(N) invariant superfluid

Yi‐Cai Zhang, Shizhong Zhang

Abstract In this paper, we develop an appropriate set of hydrodynamic equations for a U(N) invariant superfluid that couple the dynamics of superflow and magnetization. In the special case when both the superfluid and normal velocities are zero, the hydrodynamic equations reduce to a generalized version of Landau–Lifshitz equation for ferromagnetism with U(N) symmetry. When both velocities are non-zero, there appears couplings between the superflow and magnetization dynamics, and the superfluid velocity no longer satisfies the irrotational condition. On the other hand, the magnitude of magnetization is no longer a constant of motion as was the case for the standard Landau–Lifshitz theory. In comparison with the simple superfluid, the first and second sounds are modified by a non-zero magnetization through various thermodynamic functions. For U(2) invariant superfluid, we get both (zero-) sound wave and a spin wave at zero temperature. It is found that the dispersion of spin wave is always quadratic, which is consistent with microscopic analysis. In the appendix, we show that the hydrodynamic equation for a U(N) invariant superfluid can be obtained from the general hydrodynamic equation with arbitrary internal symmetries.

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Temperature-induced decay of persistent currents in a superfluid ultracold gas

Avinash Kumar, Stephen Eckel, Fred Jendrzejewski +1 more

We study how temperature affects the lifetime of a quantized, persistent current state in a toroidal Bose-Einstein condensate. When the temperature is increased, we find a decrease in the persistent current lifetime. Comparing our measured decay rates to simple models of thermal activation and quantum tunneling, we do not find agreement. We also measured the size of the hysteresis loops in our superfluid ring as a function of temperature, enabling us to extract the critical velocity. The measured critical velocity is found to depend strongly on temperature, approaching the zero-temperature mean-field solution as the temperature is decreased. This indicates that an appropriate definition of critical velocity must incorporate the role of thermal fluctuations, something not explicitly contained in traditional theories.

arXiv:1608.02894•Physical Review A•Feb 24, 2017•35 citations

Superfluid tunneling

F. Barranco, P. F. Bortignon, A. Bracco +4 more

•Jan 1, 1991•0 citations
A rotating ultracold SSS-wave superfluid Fermi gas is studied when the mismatch in chemical potentials $\ensuremath{\delta}\ensuremath{\mu}$ (and the population imbalance $\ensuremath{\delta}n$) corresponds to the Larkin-Ovchinnikov-Fulde-Ferrell state in the vicinity of the Lifshitz critical point. It is shown that under these conditions the critical angular velocity ${\ensuremath{\Omega}}_{c2}$ in two-dimensional systems is an oscillating function of temperature and $\ensuremath{\delta}n$ giving rise to reentrant superfluid phases. The reason for this behavior is the population by Cooper pairs of the Landau levels $(n\ensuremath{\ge}1)$ above the lowest one (n=0)(n=0)(n=0).
Abstract In this paper, we develop an appropriate set of hydrodynamic equations for a U(N) invariant superfluid that couple the dynamics of superflow and magnetization. In the special case when both the superfluid and normal velocities are zero, the hydrodynamic equations reduce to a generalized version of Landau–Lifshitz equation for ferromagnetism with U(N) symmetry. When both velocities are non-zero, there appears couplings between the superflow and magnetization dynamics, and the superfluid velocity no longer satisfies the irrotational condition. On the other hand, the magnitude of magnetization is no longer a constant of motion as was the case for the standard Landau–Lifshitz theory. In comparison with the simple superfluid, the first and second sounds are modified by a non-zero magnetization through various thermodynamic functions. For U(2) invariant superfluid, we get both (zero-) sound wave and a spin wave at zero temperature. It is found that the dispersion of spin wave is always quadratic, which is consistent with microscopic analysis. In the appendix, we show that the hydrodynamic equation for a U(N) invariant superfluid can be obtained from the general hydrodynamic equation with arbitrary internal symmetries.
We study how temperature affects the lifetime of a quantized, persistent current state in a toroidal Bose-Einstein condensate. When the temperature is increased, we find a decrease in the persistent current lifetime. Comparing our measured decay rates to simple models of thermal activation and quantum tunneling, we do not find agreement. We also measured the size of the hysteresis loops in our superfluid ring as a function of temperature, enabling us to extract the critical velocity. The measured critical velocity is found to depend strongly on temperature, approaching the zero-temperature mean-field solution as the temperature is decreased. This indicates that an appropriate definition of critical velocity must incorporate the role of thermal fluctuations, something not explicitly contained in traditional theories.