Bardasis-Schrieffer-like phase mode in a superconducting bilayer
arXiv:2306.16611 · doi:10.1103/PhysRevB.108.L220505
Abstract
We theoretically study the low-lying collective modes of an even-parity spin-singlet superconducting bilayer, where strong spin-orbit coupling leads to a closely competing odd-parity pairing state. We develop a gauge-invariant theory for the coupling of phase fluctuations to an external electromagnetic field and show that the competing odd-parity pairing instability gives rise to a Bardasis-Schrieffer-like phase mode within the excitation gap. Accounting for the long-range Coulomb interaction, however, we find that this mode is converted into an antisymmetric plasmon and is likely pushed into the quasiparticle continuum.
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- Field-induced superconductivity mediated by odd-parity multipole fluctuation
- Superconducting meron phase in locally noncentrosymmetric superconductors
- Collective modes in superconductors including Coulomb repulsion