HIGHLIGHTS
SUMMARY
In these superconducting materials, vortices can show an inversion of the magnetic_field away from the vortex core and new compact states that are the superconducting counterparts of the Chandrasekhar-Kendall states in highly conducting plasmas. This current, directed along the magnetic_field, stems from the breaking of parity in a non-equilibrium state and is thus a direct analog of the Chiral Magnetic Effect predicted for systems of chiral fermions and observed in Dirac and Weyl semimetals. Using h̄=c=1, the Ginzburg-Landau free_energy describing the superconducting state of non-centrosymmetric material reads as . . .
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