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 \(\lambda\) (London penetration depth) from the core. Note that in type-II superconductors \(\lambda>\xi\). The circulating supercurrents induce magnetic fields with the total flux equal to a single flux quantum \(\Phi_0\). 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
where \(K_0(z)\) is a zeroth-order Bessel function. Note that, according to the above formula, at \(r \to 0\) the magnetic field \(B(r)\propto\ln(\lambda/r)\), i.e. logarithmically diverges. In reality, for \(r\lesssim\xi\) the field is simply given by
where κ = λ/ξ is known as the Ginzburg-Landau parameter, which must be \(\kappa>1/\sqrt{2}\) 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 lower critical field \(H_{c1}\) (but smaller than the upper critical field \(H_{c2}\)), the field penetrates into superconductor in terms of Abrikosov vortices. Each vortex carries one thread of magnetic field with the flux \(\Phi_0\). 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.
See also
- Ginzburg-Landau theory
- Type-II superconductor
- Alexei Alexeyevich Abrikosov
- Macroscopic quantum phenomena
- Pinning force
- Flux pinning
References
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