Dissipation due to bulk localized low-energy modes in strongly disordered superconductors
Authors
Anton V. Khvalyuk, Mikhail V. Feigel'man
Abstract
We develop a theory of the temperature and frequency dependence of ac dissipation in strongly disordered superconductors featuring a pseudogap in the single-particle spectrum. Our theory applies to the regime , where is the typical superconducting gap. The dissipation is expressed in terms of the quality factor of microwave resonators made of these materials. We show that low- dissipation is dominated by a new type of bulk localized collective modes. Due to the strongly nonuniform spectral density of these modes, decreases sharply with frequency, while its temperature dependence exhibits a two-level-system-like growth as a function of for . Our theory is applicable to InO, TiN, NbN, and similar strongly disordered materials. We further argue that the experimentally observed behavior of disordered films of granular Aluminum is explained by similar physics, although this case requires a separate theoretical analysis.