Generalized Josephson plasmons in bilayer superconductors

Layered superconductors like High-Tc cuprates display out-of-plane plasma oscillations between layers sustained by the weak Josephson coupling among the superconducting sheets, the so-called Josephson plasmons. Bilayer cuprates hosts two of such modes, but due to the anisotropy of the electronic response their description at generic wavevector cannot be separated from that of the in-plane oscillations. In this paper we provide an analytical theoretical framework able to describe the dispersions and the polarizations of the generalized plasma modes of such systems, that has been only partly addressed by previous work in the literature. We then employ it to explain the peculiar characteristics of their linear optical response, by providing a fully microscopic explanation for the appearance of a finite-frequency peak in the real part of the optical conductivity. On a wider perspective, the complete characterization of the Josephson plasma modes provided by our approach represents a groundwork to address open issues raised by recent experiments with strong THz pulses, able to drive them beyond the linear-response regime.Comment: 21 pages, 8 figure

Manipulating Plasma Excitations with Terahertz Light Pulses in Superconducting Cuprates

Layered cuprates offer a preferential playground for optical non-linearity thanks to the emergence, below Tc, of soft out-of-plane Josephson plasmons. The hallmark of such a non-linearity is the observation of Third Harmonic Generation, that has been theoretically understood as a sum-frequency process involving a two-plasmon excitation. However, recent experiments in cuprates with two planes per unit cell challenge this interpretation, due to the lack of resonant response at the temperature where the driving frequency matches the plasma energy scale, as observed instead in single-layer cuprates. Here we show that such an apparent discrepancy in bilayer systems can be resolved by taking into account the combined effect of light polarization and Josephson-coupling anisotropy on setting the energy range where three-dimensional layered plasma modes can be resonantly excited. Our results offer a novel perspective on the possibility to tune on demand high-harmonic generation by artificially designing Josephson heterostructures