Abrikosov vortex

---

title: "Abrikosov vortex" type: doc version: 1 created: 2026-02-28 author: "Wikipedia contributors" status: active scope: public tags: ["superconductivity", "vortices"] description: "Vortex of supercurrent within a type-II superconductor" topic_path: "general/superconductivity" source: "https://en.wikipedia.org/wiki/Abrikosov_vortex" license: "CC BY-SA 4.0" wikipedia_page_id: 0 wikipedia_revision_id: 0

::summary Vortex of supercurrent within a type-II superconductor ::

::figure[src="https://upload.wikimedia.org/wikipedia/commons/7/7d/YBCO_vortices.jpg" caption="arxiv=1807.06746}}"] ::

In superconductivity, a fluxon (also called an Abrikosov vortex or quantum vortex) is a vortex of supercurrent in a type-II superconductor, used by Soviet physicist Alexei Abrikosov to explain magnetic behavior of type-II superconductors. Abrikosov vortices occur generically in the Ginzburg–Landau theory of superconductivity.

Overview

The solution is a combination of fluxon solution by Fritz London, combined with a concept of core of quantum vortex by Lars Onsager.

In the quantum vortex, 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/\sqrt{2}. 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 the same equation as in the London's fluxoid 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 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

B(0)\approx \frac{\Phi_0}{2\pi\lambda^2}\ln\kappa, where κ = λ/ξ is known as the Ginzburg–Landau parameter, which must be \kappa1/\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 obeys London's magnetic flux quantization and carries one quantum of magnetic flux \Phi_0. Abrikosov vortices form a lattice, usually triangular (of hexagonal symmetry), with the average vortex density (flux density) approximately equal to the externally applied magnetic field. As with other lattices, defects may form as dislocations.

References

References

1. (2015). "Analysis of low-field isotropic vortex glass containing vortex groups in YBa₂Cu₃O_7−x thin films visualized by scanning SQUID microscopy". Scientific Reports.
2. (1957). "The magnetic properties of superconducting alloys". [[Journal of Physics and Chemistry of Solids]].
3. Onsager, L.. (March 1949). "Statistical hydrodynamics". Il Nuovo Cimento.
4. Feynman, R.P.. (1955). "Chapter II Application of Quantum Mechanics to Liquid Helium". Elsevier.
5. London, F.. (1948-09-01). "On the Problem of the Molecular Theory of Superconductivity". Physical Review.
6. London, Fritz. (1961). "Superfluids". Dover.
7. de Gennes, Pierre-Gilles. (2018). "Superconductivity of Metals and Alloys". Addison Wesley Publishing Company, Inc.

::callout[type=info title="Wikipedia Source"] This article was imported from Wikipedia and is available under the Creative Commons Attribution-ShareAlike 4.0 License. Content has been adapted to SurfDoc format. Original contributors can be found on the article history page. ::