Cavity Quantum Eliashberg Enhancement of Superconductivity

Driving a conventional superconductor with an appropriately tuned classical electromagnetic field can lead to an enhancement of superconductivity via a redistribution of the quasiparticles into a more favorable non-equilibrium distribution -- a phenomenon known as the Eliashberg effect. Here we theoretically consider coupling a two-dimensional superconducting film to the quantized electromagnetic modes of a microwave resonator cavity. Within the weak cavity-coupling regime, we compute the rate of Bogoliubov quasiparticle pair creation (annihilation) through photon absorption (emission) processes. Both a clean and disordered superconductor are considered. Using a kinetic equation in the presence of inelastic relaxation processes, we compute the non-thermal distribution of Bogoliubov excitations. It is shown that the photons serve to preferentially cool the quasiparticles residing near the gap edge, leading to an enhancement of the BCS gap. To conclude, we comment on the strong cavity-coupling regime, where formation of Bogoliubov-polaritons due to hybridization between photons and pairs of Bogoliubov quasiparticles may be possible.