Anomalous gap-edge dissipation in disordered superconductors on the brink of localization

Cheng, Bing ; Wu, Liang ; Laurita, N. J. ; Singh, Harkirat ; Chand, Madhavi ; Raychaudhuri, Pratap ; Armitage, N. P. (2016) Anomalous gap-edge dissipation in disordered superconductors on the brink of localization Physical Review B: Condensed Matter and Materials Physics, 93 (18). p. 180511. ISSN 1098-0121

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Official URL: https://journals.aps.org/prb/abstract/10.1103/Phys...

Related URL: http://dx.doi.org/10.1103/PhysRevB.93.180511

Abstract

Superconductivity in disordered systems close to an incipient localization transition has been an area of investigation for many years, but many fundamentally important aspects are still not understood. It has been noted that in such highly disordered superconductors, anomalous spectral weight develops in their conductivity near and below the superconducting gap energy. In this work we investigate the low frequency conductivity in disordered superconducting NbN thin films close to the localization transition with time-domain terahertz spectroscopy. In the normal state, strong deviations from the Drude form due to incipient localization are found. In the superconducting state we find substantial spectral weight at frequencies well below the superconducting gap scale derived from tunneling. We analyze this spectral weight in the context of a model of disorder induced broadening of the quasiparticle density of states. We find that aspects of the optical and tunneling data can be consistently modeled in terms of this effect of mesoscopic disorder, showing that in this disorder and frequency range, quasiparticle effects and not collective modes are the source of low energy absorption. Interestingly, we also find that as a function of frequency the optical conductivity recovers to the normal state value much faster than any model predicts. This points to the nontrivial interplay of superconductivity and disorder close to localization.

Item Type:Article
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ID Code:105239
Deposited On:25 Dec 2017 12:11
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