Conservation laws, vertex corrections, and screening in Raman spectroscopy
arXiv:1703.02170 · doi:10.1103/PhysRevB.96.014503
Abstract
We present a microscopic theory for the Raman response of a clean multiband superconductor accounting for the effects of vertex corrections and long-range Coulomb interaction. The measured Raman intensity, , is proportional to the imaginary part of the fully renormalized particle-hole correlator with Raman form-factors . In a BCS superconductor, a bare Raman bubble is non-zero for any and diverges at , where is the largest gap along the Fermi surface. However, for const, the full is expected to vanish due to particle number conservation. It was long thought that this vanishing is due to the singular screening by long-range Coulomb interaction. We argue that this vanishing actually holds due to vertex corrections from the same short-range interaction that gives rise to superconductivity. We further argue that long-range Coulomb interaction does not affect the Raman signal for . We argue that vertex corrections eliminate the divergence at and replace it with a maximum at a somewhat larger frequency. We also argue that vertex corrections give rise to sharp peaks in at , when coincides with the frequency of one of collective modes in a superconductor, e.g, Leggett mode, Bardasis-Schrieffer mode, or an excitonic mode.
19pp; 8figs; References to more old work added
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