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Optically active Higgs and Leggett modes in multiband pair-density-wave superconductors with Lifshitz invariant
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abstract
Lifshitz invariant is a symmetry invariant composed of multiple order parameters that contain a single spatial derivative in a Ginzburg-Landau (GL) free energy, which may induce a nonuniform configuration of the order parameters. In multiband superconductors, we find phase transitions from a uniform superconducting state to qualitatively distinct two pair-density-wave (PDW) states with small and large momenta $\boldsymbol{q}$ based on the GL theory. The former is induced by the Lifshitz invariant, while the latter originates from the drag effect. In the PDW states, the Higgs and Leggett modes (i.e., collective amplitude and relative phase oscillations of the order parameters) are shown to couple to electromagnetic fields linearly. We construct microscopic models of multiband superconductors with Lifshitz invariant that exhibit PDW states, and calculate the linear optical conductivity using the diagrammatic approach. We find optically active Higgs and Leggett modes in the small $\boldsymbol{q}$ PDW state, indicating that the PDW state is a suitable platform to explore collective modes of multiband superconductors in the linear response regime.
Forward citations
Cited by 2 Pith papers
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Gauge-invariant electromagnetic responses in superconductors
A gauge-invariant framework for arbitrary-order electromagnetic response in conventional and unconventional superconductors is derived from Ward identities and the gap equation.
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Time-reversal symmetry breaking, collective modes, and Raman spectrum in pair-density-wave states
Coexisting pair-density-wave and uniform d-wave superconducting order generates a sharp, Raman-active Higgs mode and breaks time-reversal symmetry.
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