Abrikosov vortex

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In superconductivity, an Abrikosov vortex is a vortex of supercurrent in a type-II superconductor. The supercurrent circulates around the normal (i.e. non-superconducting) core of the vortex. The core has a size $\sim\xi$ --- the superconducting coherence length (parameter of a Ginzburg-Landau theory). The supercurrents decay on the distance about $λ$ (London penetration depth) from the core. Note that in type-II superconductors $λ > ξ$ . The circulating supercurrents induce magnetic field with the total flux equal to a single flux quantum $Φ 0$ . Therefore, an Abrikosov vortex is often called a fluxon.

The magnetic field distribution of a single vortex far from its core can be described by

$B(r) = \frac{\Phi_0}{2\pi\lambda^2}K_0\left(\frac{r}{\lambda}\right) \approx \sqrt{\frac{\lambda}{r}} \exp\left(-\frac{r}{\lambda}\right),$

where $K 0 (z)$ is the so-called Bessel function. Note that, according to the above formula, at $r \to 0$ the magnetic field $B(r)\propto\ln(\lambda/r)$ , i.e. logariphmically diverges. In reality, for $r\lesssim\xi$ the field is simply given by

$B(0)\approx \frac{\Phi_0}{2\pi\lambda^2}\ln\kappa,$

where $κ = λ / ξ$ is a Ginsburg-Landau parameter, which must be $\kappa>\sqrt{2}$ in type-II superconductors.

Abrikosov vortices can be trapped in a type-II superconductor by chance, on defects, etc. Even if initially type-II superconductor contains no vortices, and one applies a magnetic field $H$ larger than the first critical field $H c 1$ (but smaller than the second critical field $H c 2$ ), the field penetrates into superconductor in terms of Abrikosov vortices. Each vortex carries one thread of magnetic field with the flux $Φ 0$ . Abrikosov vortices form a lattice (usually triangular, may be with defects/dislocations) with the average vortex density (flux density) approximately equal to the externally applied magnetic field.