Abstract
This Chapter gives a brief introduction to some basic aspects metals and superconductors in crystals without inversion symmetry. In the first part we analyze some normal state properties which arise through antisymmetric spin-orbit coupling existing in non-centrosymmetric materials and show its influence on the de Haas–van Alphen effect. For the superconducting phase we introduce a multi-band formulation which naturally arises due the spin splitting of the bands by spin-orbit coupling. It will then be shown how the states can be symmetry classified and their relation to the original classification in even-parity spin-singlet and odd-parity spin-triplet pairing states. The general Ginzburg–Landau functional will be derived and applied to the nucleation of superconductivity in a magnetic field. It will be shown that magneto-electric effects can modify the standard paramagnetic limiting behavior drastically.
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- 1.
The interband pairing leads to the interesting possibility of existence of nonuniform superconducting states even in the absence of external magnetic fields [52]. These states, however, could be realized in the noncentrosymmetric compounds with the SO band splitting smaller than the superconducting critical temperature. To the best of our knowledge, in all noncentrosymmetric compounds discovered to date the relation between the two energy scales is exactly the opposite: the SO band splitting exceeds all superconducting energy scales by order of magnitude, completely suppressing the interband pairing, both uniform and nonuniform.
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Mineev, V.P., Sigrist, M. (2012). Basic Theory of Superconductivity in Metals Without Inversion Center. In: Bauer, E., Sigrist, M. (eds) Non-Centrosymmetric Superconductors. Lecture Notes in Physics, vol 847. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-24624-1_4
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