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Vortices and magnetic impurities

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arxiv 1808.07441 v2 pith:4EXIR2QM submitted 2018-08-22 hep-th

classification hep-th
keywords impuritycouplingvortexvorticescriticaldependsimpuritiesaway
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Ginzburg-Landau vortices in superconductors attract or repel depending on whether the value of the coupling constant is less than 1 or larger than 1. At critical coupling it was previously observed that a strongly localised magnetic impurity behaves very similarly to a vortex. This remains true for axially symmetric configurations away from critical coupling. In particular, a delta function impurity of a suitable strength is related to a vortex configuration without impurity by singular gauge transformation. However, the interaction of vortices and impurities is more subtle and depends not only on the coupling constant and the impurity strength, but also on how broad the impurity is. Furthermore, the interaction typically depends on the distance and may be attractive at short distances and repulsive at long distances. Numerical simulations confirm moduli space approximation results for the scattering of one and two vortices with an impurity. However, a double vortex will split up when scattering with an impurity, and the direction of the split depends on the sign of the impurity. Head-on collisions of a single vortex with different impurities away from critical coupling is also briefly discussed.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Field Theory of Superconductor and Charged Vortex

    cond-mat.supr-con 2025-05 conditional novelty 7.0 of 10

    The paper proposes a Lagrangian for superconductivity with a phonon field and shows that at two critical couplings, charged vortices saturate a BPS bound at the type I/II boundary.

  2. Charged Vortex in Superconductor

    cond-mat.supr-con 2025-05 conditional novelty 5.0 of 10

    Charged, spinless vortex solutions exist in a Schrödinger-type superconductor model only at the critical phonon coupling, and become noninteracting BPS vortices at the critical quartic coupling.

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