Non-equilibrium superconductivity in quantum-sensing superconducting resonators

• Published in: Superconductor science & technology Vol. 26; no. 1; pp. 15004 - 1-10
• Main Authors: Goldie, D J, Withington, S
• Format: Journal Article
• Language: English
• Published: Bristol IOP Publishing 01.01.2013; Institute of Physics
• Subjects: Bolometer; infrared, submillimeter wave, microwave and radiowave receivers and detectors; Condensed matter: electronic structure, electrical, magnetic, and optical properties; Density; Detectors; Exact sciences and technology; Infrared, submillimeter wave, microwave and radiowave instruments, equipment and techniques; Instruments, apparatus, components and techniques common to several branches of physics and astronomy; Mathematical models; Microwave probes; Microwaves; Physics; Resonators; Superconducting materials (excluding high-tc compounds); Superconductivity; Superconductors; Frequency dependence; Pair breaking; Superconducting transitions; Precision engineering; Phonons; Superconductivity; Background noise; Quasiparticles; Kinetic equations; Quality factor; Microwave resonator; Quantum detector; Superconducting resonators
• DOI: 10.1088/0953-2048/26/1/015004
• ISSN: 0953-2048

Low temperature microwave superconducting resonators (SRs) are attractive candidates for producing quantum-sensitive, arrayable energy or power detectors for astrophysical and other precision measurement applications. Their readout uses a microwave probe signal with quanta of energy well below the threshold for pair-breaking in the superconductor. We have calculated the non-equilibrium quasiparticle and phonon distributions generated by the photons of the probe signal of a resonator operating well below its superconducting transition temperature Tc as the absorbed probe power was changed using the coupled kinetic equations described by Chang and Scalapino. The calculations give insight into a rate equation estimate which suggests that the quasiparticle distributions can be driven far from their thermal equilibrium value for typical readout powers. From the driven quasiparticle distribution functions, the driven quasiparticle number densities and lifetimes were calculated. An effective temperature to describe the driven quasiparticles was defined. The non-equilibrium lifetimes were compared to the distribution-averaged thermal lifetimes at the effective temperature and good agreement was found typically within a few per cent. We used the non-equilibrium quasiparticle distribution to model a representative SR. The complex conductivity and hence the frequency dependence of the experimentally measured forward scattering parameter S21 of the SR as a function of absorbed power were found. The non-equilibrium S21 cannot be accurately modeled by a thermal distribution even at its own elevated temperature, having a higher quality factor in all cases studied, although for low absorbed powers the two effective temperatures are similar. From the non-equilibrium lifetimes and number densities we determined the achievable noise equivalent power (NEP) of the resonator used as a power detector as a function of absorbed microwave power. Simpler expressions to evaluate the effective quasiparticle temperature as a function of absorbed power have also been derived. We conclude that multiple photon absorption from the microwave probe increases the quasiparticle number above the thermal background and ultimately limits the achievable NEP of the resonator at temperatures well below Tc.