Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Dynamics of superfluid vorticity in nondissipative processes

Daniel Lhuillier, Marianne Francois

Published May 21, 1973• 0 citations
OpenAlex

Related papers

Dynamical properties of vortices in superfluid systems

Ertugrul Demircan

•Jan 1, 1997•0 citations

Dynamics of quantized vortices in rotating superfluid

Makoto Tsubota, Hideki Yoneda

Journal of Low Temperature Physics•Nov 1, 1995•13 citations

Hidden vortex lattices in a thermally paired superfluid

E. K. Dahl, Egor S. Babaev, Asle Sudbø

We study the evolution of rotational response of a statistical mechanical model of two-component superfluid with a nondissipative drag interaction as the system undergoes a transition into a paired superfluid phase at finite temperature. The transition manifests itself in a change of (i) vortex-lattice symmetry and (ii) nature of the vortex state. Instead of a vortex lattice, the system forms a highly disordered tangle which constantly undergoes merger and reconnecting processes involving different types of vortices with a ``hidden'' breakdown of translation symmetry.

arXiv:0807.0233•Physical Review B•Oct 15, 2008•17 citations

Vortex dynamics in superfluid systems

Carlos Wexler

•Jan 1, 1997•1 citation

Experiments on the Dynamics of Vortices in Superfluid 4He with No Normal Component

Paul M. Walmsley, А. А. Левченко, Andrei I. Golov

Journal of Low Temperature Physics•Nov 21, 2006•9 citations

Shear Flow and Kelvin-Helmholtz Instability in Superfluids

R. Blaauwgeers, V. B. Eltsov, Georg Eska +6 more

The first realization of instabilities in the shear flow between two superfluids is examined. The interface separating the A and B phases of superfluid 3He is magnetically stabilized. With uniform rotation we create a state with discontinuous tangential velocities at the interface, supported by the difference in quantized vorticity in the two phases. This state remains stable and nondissipative to high relative velocities, but finally undergoes an instability when an interfacial mode is excited and some vortices cross the phase boundary. The measured properties of the instability are consistent with the classic Kelvin-Helmholtz theory when modified for two-fluid hydrodynamics.

arXiv:cond-mat/0111343•Physical Review Letters•Sep 20, 2002•182 citations
We study the evolution of rotational response of a statistical mechanical model of two-component superfluid with a nondissipative drag interaction as the system undergoes a transition into a paired superfluid phase at finite temperature. The transition manifests itself in a change of (i) vortex-lattice symmetry and (ii) nature of the vortex state. Instead of a vortex lattice, the system forms a highly disordered tangle which constantly undergoes merger and reconnecting processes involving different types of vortices with a ``hidden'' breakdown of translation symmetry.
The first realization of instabilities in the shear flow between two superfluids is examined. The interface separating the A and B phases of superfluid 3He is magnetically stabilized. With uniform rotation we create a state with discontinuous tangential velocities at the interface, supported by the difference in quantized vorticity in the two phases. This state remains stable and nondissipative to high relative velocities, but finally undergoes an instability when an interfacial mode is excited and some vortices cross the phase boundary. The measured properties of the instability are consistent with the classic Kelvin-Helmholtz theory when modified for two-fluid hydrodynamics.