{ "id": "2210.04842", "version": "v1", "published": "2022-10-10T16:59:04.000Z", "updated": "2022-10-10T16:59:04.000Z", "title": "Loss and decoherence at the quantum Hall - superconductor interface", "authors": [ "Lingfei Zhao", "Zubair Iftikhar", "Trevyn F. Q. Larson", "Ethan G. Arnault", "Kenji Watanabe", "Takashi Taniguchi", "Francois Amet", "Gleb Finkelstein" ], "categories": [ "cond-mat.mes-hall", "cond-mat.supr-con" ], "abstract": "High quality type-II superconducting contacts have recently been developed to a variety of 2D systems, allowing one to explore the superconducting proximity in the quantum Hall (QH) regime. Inducing superconducting correlations into a chiral system has long been viewed as a route for creating exotic topological states and excitations. However, it appears that before these exciting predictions could be realized, one should develop a better understanding of the limitations imposed by the physics of real materials. Here, we perform a systematic study of Andreev conversion at the interface between a superconductor and graphene in the QH regime. We find that the probability of Andreev conversion of electrons to holes follows an unexpected but clear trend: the dependencies on temperature and magnetic field are nearly decoupled. We discuss these trends and the role of the superconducting vortices, whose normal cores could both absorb and dephase the individual electrons in a QH edge. Our study may pave the road to engineering future generation of hybrid devices for exploiting superconductivity proximity in chiral channels.", "revisions": [ { "version": "v1", "updated": "2022-10-10T16:59:04.000Z" } ], "analyses": { "keywords": [ "quantum hall", "superconductor interface", "decoherence", "high quality type-ii superconducting contacts", "andreev conversion" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }