{ "id": "2002.05590", "version": "v1", "published": "2020-02-13T16:07:44.000Z", "updated": "2020-02-13T16:07:44.000Z", "title": "Weak localization corrections to the thermal conductivity in $s$-wave superconductors", "authors": [ "Lucia Gonzalez Rosado", "Fabian Hassler", "Gianluigi Catelani" ], "comment": "15 pages, 6 figures", "categories": [ "cond-mat.mes-hall", "cond-mat.dis-nn", "cond-mat.supr-con" ], "abstract": "We study the thermal conductivity in disordered $s$-wave superconductors. Expanding on previous works for normal metals, we develop a formalism that tackles particle diffusion as well as the weak localization (WL) and weak anti-localization (WAL) effects. Using a Green's functions diagrammatic technique, which takes into account the superconducting nature of the system by working in Nambu space, we identify the system's low-energy modes, the diffuson and the Cooperon. The time scales that characterize the diffusive regime are energy dependent; this is in contrast with the the normal state, where the relevant time scale is the mean free time $\\tau_e$, independent of energy. The energy dependence introduces a novel energy scale $\\varepsilon_*$, which in disordered superconductors ($\\tau_e \\Delta\\ll 1$, with $\\Delta$ the gap) is given by $\\varepsilon_* = \\sqrt{\\Delta/\\tau_e}$. From the diffusive behavior of the low-energy modes, we obtain the WL correction to the thermal conductivity. We give explicitly expressions in two dimensions. We determine the regimes in which the correction depends explicitly on $\\varepsilon_*$ and propose an optimal regime to verify our results in an experiment.", "revisions": [ { "version": "v1", "updated": "2020-02-13T16:07:44.000Z" } ], "analyses": { "keywords": [ "thermal conductivity", "weak localization corrections", "wave superconductors", "greens functions diagrammatic technique", "relevant time scale" ], "note": { "typesetting": "TeX", "pages": 15, "language": "en", "license": "arXiv", "status": "editable" } } }