Leggett modes and the Anderson-Higgs mechanism in superconductors without inversion symmetry
arXiv:1503.08133 · doi:10.1103/PhysRevLett.115.227002
Abstract
We develop a microscopic and gauge-invariant theory for collective modes resulting from the phase of the superconducting order parameter in non-centrosymmetric superconductors. Considering various crystal symmetries we derive the corresponding gauge mode and find, in particular, new Leggett modes with characteristic properties that are unique to non-centrosymmetric superconductors. We calculate their mass and dispersion that reflect the underlying spin-orbit coupling and thus the balance between triplet and singlet superconductivity occurring simultaneously. Finally, we demonstrate the role of the Anderson-Higgs mechanism: while the long-range Coulomb interaction shifts to the condensate plasma mode , it leaves the mass of the new Leggett mode unaffected and only slightly modifies its dispersion.
10 pages, 3 figures
References in corpus (4)
- Observation of Leggett's collective mode in a multi-band MgB2 superconductor
- Gap structure in noncentrosymmetric superconductors
- Electronic Raman scattering in non-centrosymmetric superconductors
- Macroscopic quantum tunneling in multigap superconducting Josephson junctions: Escape rate enhancement via quantum fluctuations of Josephson-Leggett mode
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