In very anisotropic
layered superconductors tilted magnetic field generates two interpenetrating
vortex sublattices. This set of crossing lattices contains a sublattice of
Josephson vortices and a sublattice of pancake-vortex stacks. The
pancake-vortex sublattice modifies structure of the Josephson vortex in a very
unusual way. Josephson
vortex induces deformations in the pancake vortex crystal, which, in turn,
substantially modify the Josephson vortex structure. The phase field of
the Josephson vortex is composed of two types of phase deformations: the
regular phase and vortex phase. The phase deformations with smaller stiffness
dominate. The contribution from the vortex phase smoothly takes over with
increasing magnetic field. The core structure depends on the ratio of
the London penetration depth l and
the bare size of Josephson vortex core lJ
and experiences a smooth yet qualitative evolution with increase of this
ratio. At small ratios l/lJ
pancakes have only small deformations with respect to position of the
ideal crystal (see upper structure in the Figure), while at higher ratios
the pancake stacks in the central row smoothly transfer between the neighboring
lattice positions forming a solitonlike structure (see lower structure
in the Figure). |
![]() Figure: Structure of the in-plane vortex inside the pancake lattice for two values of the ratio l/lJ. Left column shows graylevel plot of the cosine of the interlayer phase difference and right column shows pancake coordinates in the central row. | |
| For details see Phys. Rev. B, 68 094520 (2003) | ||