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Flux lines in type II superconductors


In a type II superconductor, an external magnetic field applied to a sample penetrates in the form of quantized bundles of flux, known as flux or vortex lines[8]. These flux bundles are in fact topological defects very analogous to domain walls in Ising magnets. In the case of the superconductor, the order parameter is the complex ``pair wavefunction'' or gap


The macroscopic properties of most superconductors are well described by a phenomenological expansion of the free energy in tex2html_wrap_inline3288 coupled to the electro-magnetic field, known as Ginzburg-Landau theory


where tex2html_wrap_inline3290 , tex2html_wrap_inline3292 is the superconducting flux quantum. The factor of 2e in tex2html_wrap_inline3296 reflects the charge of the singlet pair.

In the ordered phase at low temperatures, the coefficient tex2html_wrap_inline3298 is large and negative, and tex2html_wrap_inline3288 develops an almost uniform amplitude. tex2html_wrap_inline3302 . The phase, however, can still vary in space,


Up to a constant, the free energy becomes


A vortex is a configuration of tex2html_wrap_inline2978 which winds by tex2html_wrap_inline2792 around some closed loop enclosing a singularity in the phase field (a singularity is necessary since the phase must wind even as one shrinks the path to a point). In three dimensions, these singularities take the form of lines.

Let us now examine the magnetic flux passing through such a loop. At low temperatures, minimization of Eq. 115 requires


which, when integrated around the loop implies


Since the integral on the right hand side is just the flux through the loop, we have


Each vortex line therefore carries a quantum of magnetic flux (in fact, one may imagine vortex configurations with larger winding numbers, but these turn out to be energetically unfavorable, and split spontaneously into collections of fundamental vortices).

The density of vortices in the superconductor is determined by the magnitude of the applied field. Away from extremely low fields, where screening effects can be important, the vortex density adjusts so that there is one flux line per flux quantum, i.e.


where n is the areal density of vortex lines. If the magnetic field is fairly low, we may attempt to treat the vortices as independent. We'll return to the question of the behavior of the bulk system later.

If we assign an energy cost tex2html_wrap_inline3310 per unit length of the line, a gradient expansion leads naturally to the random manifold elastic energy (with d=1),


Disorder is always present in the form of atomic defects (probably dominant are oxygen vacancies in the doped cuprates) and larger defects such as grain boundaries, twin plans, screw dislocations... We will focus on the more microscopic point defects modeled phenomenologically by the random potential V.

So the vortex lines fit reasonably well into the framework of random manifolds. We therefore expect similar overall behavior, including the extremely slow response to an applied force. This is very important for the superconductors, because vortex motion is the main source of dissipation in these materials.

To understand this, suppose we run a (super) current through the superconductor, perpendicular to the magnetic field axis. Because the vortices carry a magnetic field, they exert a tex2html_wrap_inline3316 force on the current. By Newton's third law, the vortices therefore experience an equal and opposite force,


. known as the Lorentz force. In the absence of disorder, this will cause the vortex to move in the direction perpendicular to both tex2html_wrap_inline3318 and tex2html_wrap_inline3320 . Assuming a constant mobility tex2html_wrap_inline3322 (i.e. damping) for the vortex, the asymptotic velocity


Since the vortex is magnetic, however this means that the system now has a time-varying magnetic field. By Faraday's law, this induces an electric field parallel to the current


The system therefore has a non-zero longitudinal dissipative resistivity.

When disorder is present, the vortices are pinned, and the effective mobility tex2html_wrap_inline3322 is drastically reduced. In fact, since we expect v to be exponentially small in f, the linear resistivity vanishes! This slow ``creep'' motion discussed earlier was actually first suggested in the context of flux motion in superconductors.

next up previous contents
Next: Relation to surface growth Up: Directed polymers Previous: Directed polymers

Leon Balents
Thu May 30 08:21:44 PDT 1996