Strong-coupling and the Stripe phase of He
arXiv:1605.01047 · doi:10.1007/s10909-016-1632-7
Abstract
Thin films of superfluid He were predicted, based on weak-coupling BCS theory, to have a stable phase which spontaneously breaks translational symmetry in the plane of the film. This crystalline superfluid, or "stripe" phase, develops as a one dimensional periodic array of domain walls separating degenerate B phase domains. We report calculations of the phases and phase diagram for superfluid He in thin films using a strong-coupling Ginzburg-Landau theory that accurately reproduces the bulk He superfluid phase diagram. We find that the stability of the Stripe phase is diminished relative to the A phase, but the Stripe phase is stable in a large range of temperatures, pressures, confinement, and surface conditions.
arXiv comment9 pages, 11 figures
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- Half-Quantum Vortices in Nematic and Chiral Phases of He
- Radial Fulde-Ferrell-Larkin-Ovchinnikov state in a population-imbalanced Fermi gas
- A-B transition in superfluid He and cosmological phase transitions
- Feasibility of a Fulde-Ferrell-Larkin-Ovchinnikov superfluid Fermi atomic gas
- Weyl Fermions and Broken Symmetry Phases of Laterally Confined He Films
- Effects of a magnetic field on vortex states in superfluid He-B
- Strong-coupling corrections to hard domain walls in superfluid 3He-B
- Superfluid phase transition of nanoscale-confined helium-3
- Kibble-Zurek Dynamics & Statistics of Topological Defects in Chiral Superfluid He Films
- Dimensional crossover of superfluid He in a magnetic field
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