Dimensional crossover of superfluid He in a magnetic field
arXiv:2507.10763 · doi:10.1103/jfwt-f3bw
Abstract
Motivated by recent experiments on superfluid He in nanoscale-confined geometries, we theoretically investigate the associated phase diagram in a slab geometry and perpendicular magnetic field as the size of confinement is varied. Our analysis is based on minimizing the Ginzburg--Landau free energy for the matrix superfluid order parameter for three different boundary conditions. We observe a smooth crossover from the phase diagram of the 3D system to the quasi-2D limit for slab heights of several hundred nanometres and magnetic fields of several kilogauss. We illuminate that, despite the apparent complexity of the underlying equations, many precise numerical and even analytical statements can be made about the phase structure for general values of the coefficients of the free energy functional, which can in turn be used to constrain or measure these parameters. To guide future experimental studies, we compute the phase diagram in dependence of pressure, temperature, slab height, and magnetic field.
arXiv comment37 pages
References in corpus (29)
- Paired states of fermions in two dimensions with breaking of parity and time-reversal symmetries, and the fractional quantum Hall effect
- The Physics of Pair Density Waves
- Emergent Space-time Supersymmetry at the Boundary of a Topological Phase
- The Fulde-Ferrell-Larkin-Ovchinnikov state for ultracold fermions in lattice and harmonic potentials: a review
- Symmetry Protected Topological Superfluids and Superconductors --- From the Basics to He ---
- Symmetry Protected Topological Order and Spin Susceptibility in Superfluid 3He-B
- Crystalline order in superfluid 3He films
- Unconventional Superconductivity in Luttinger Semimetals: Theory of Complex Tensor Order and the Emergence of the Uniaxial Nematic State
- Evidence for a Spatially-Modulated Superfluid Phase of He under Confinement
- Phase structure of mass- and spin-imbalanced unitary Fermi gases
- Stabilized Pair Density Wave via Nanoscale Confinement of Superfluid He
- Strong Coupling Corrections to the Ginzburg-Landau Theory of Superfluid ^{3}He
- Symmetry Protected Topological Superfluid He-B
- Superfluid phases of He in nano-scale channels
- Superfluid 3He in a restricted geometry with a perpendicular magnetic field
- Fragility of surface states in topological superfluid He
- Strong-coupling and the Stripe phase of He
- Renormalization theory for the Fulde-Ferrell-Larkin-Ovchinnikov states at
- Sarma phase in relativistic and non-relativistic systems
- Superfluid phases of He in a periodic confined geometry
- Triangular pair density wave in confined superfluid He
- Domain Walls in Superfluid 3He-B
- Ground state of the three-dimensional BCS d-wave superconductor
- Surface State Dissipation in Confined 3He-A
- Strong-coupling corrections to hard domain walls in superfluid 3He-B
- Superfluid phase transition of nanoscale-confined helium-3
- Competition of vortex core structures in superfluid He-B
- p-wave superconductivity and the axi-planar phase of triple-point fermions
- Chiral superfluid helium-3 in the quasi-two-dimensional limit