Ginzburg-Landau Vortex Lattice in Superconductor Films of Finite Thickness
arXiv:cond-mat/0409779 · doi:10.1103/PhysRevB.71.014521
Abstract
The Ginzburg-Landau equations are solved for ideally periodic vortex lattices in superconducting films of arbitrary thickness in a perpendicular magnetic field. The order parameter, current density, magnetic moment, and the 3-dimensional magnetic field inside and outside the film are obtained in the entire ranges of the applied magnetic field, Ginzburg Landau parameter kappa, and film thickness. The superconducting order parameter varies very little near the surface (by about 0.01) and the energy of the film surface is small. The shear modulus c66 of the triangular vortex lattice in thin films coincides with the bulk c66 taken at large kappa. In thin type-I superconductor films with kappa < 0.707, c66 can be positive at low fields and negative at high fields.
12 pages including 14 Figures, corrected, Fig.14 added, appears in Phys. Rev. B 71, issue 1 (2005)
References in corpus (1)
Cited by in corpus (12)
- Scanning superconducting quantum interference device on a tip for magnetic imaging of nanoscale phenomena
- Thin superconductors and SQUIDs in perpendicular magnetic field
- Critical current scaling and anisotropy in oxypnictide superconductors
- Ground State and Tkachenko Modes of a Rapidly Rotating Bose-Einstein Condensate in the Lowest Landau Level State
- Vortex-vortex interaction in thin superconducting films
- Direct evidence of superconductivity and determination of the superfluid density in buried ultrathin FeSe grown on SrTiO
- Giant vortex states in type I superconductors simulated by Ginzburg-Landau equations
- Muon Spin Rotation and the Vortex Lattice in Superconductors
- Doubly Quantized Vortices in Bulk Ginzburg-Landau Superconductors
- Simple Vortex States in Films of Type-I Ginzburg-Landau Superconductor
- Surface deformation caused by the Abrikosov vortex lattice
- Topological defects in superconducting open nanotubes under gradual and abrupt switch-on of the transport current and magnetic field