Tunable Klein-like tunnelling of high-temperature superconductor pairs into graphene

Superconductivity can be induced in a normal material via the ‘leakage’ of superconducting pairs of charge carriers from an adjacent superconductor. This so-called proximity e ect is markedly influenced by graphene’s unique electronic structure, both in fundamental and technologically relevant ways....

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Detalles Bibliográficos
Autores: Perconte, David, Cuéllar Jiménez, Fabian Andrés, Moreau-Luchaire, Constance, Piquemail-Banci, Maelis, Galceran, Regina, Kidambi, Piran R., Martin, Marie-Blandine, Hofmann, Stephan, Bernard, Rozenn, Dlubak, Bruno, Seneor, Pierre, Villegas Hernández, Javier Eulogio
Tipo de recurso: artículo
Fecha de publicación:2017
País:España
Institución:Universidad Complutense de Madrid (UCM)
Repositorio:Docta Complutense
Idioma:inglés
OAI Identifier:oai:docta.ucm.es:20.500.14352/99411
Acceso en línea:https://hdl.handle.net/20.500.14352/99411
Access Level:acceso abierto
Palabra clave:538
Graphene
Klein tunneling
Superconductor
Física de materiales
2211.11 Propiedades de Transporte de Electrones
2211.26 Dispositivos de Estado Sólido
2211.27 Superconductores
Descripción
Sumario:Superconductivity can be induced in a normal material via the ‘leakage’ of superconducting pairs of charge carriers from an adjacent superconductor. This so-called proximity e ect is markedly influenced by graphene’s unique electronic structure, both in fundamental and technologically relevant ways. These include an unconventional form1,2 of the ‘leakage’ mechanism— the Andreev reflection3—and the potential of supercurrent modulation through electrical gating4 . Despite the interest of high-temperature superconductors in that context5,6 , realizations have been exclusively based on low-temperature ones. Here we demonstrate a gate-tunable, high-temperature superconducting proximity e ect in graphene. Notably, gating e ects result from the perfect transmission of superconducting pairs across an energy barrier—a form of Klein tunnelling7,8 , up to now observed only for non-superconducting carriers9,10— and quantum interferences controlled by graphene doping. Interestingly, we find that this type of interference becomes dominant without the need of ultraclean graphene, in stark contrast to the case of low-temperature superconductors11. These results pave the way to a new class of tunable, high-temperature Josephson devices based on large-scale graphene.