Manipulating the topological interface by molecular adsorbates

Topological insulators are a promising class of materials for applications in the field of spintronics. New perspectives in this field can arise from interfacing metal-organic molecules with the topological insulator spin-momentum locked surface states, which can be perturbed enhancing or suppressin...

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Detalles Bibliográficos
Autores: Caputo, Marco, Panighel, Mirco|||0000-0001-8413-5196, Lisi, Simone, Khalil, Lama, Santo, Giovanni Di, Papalazarou, Evangelos, Hruban, Andrzej, Konczykowski, Marcin, Krusin-Elbaum, Lia, Aliev, Ziya S., Babanly, Mahammad B., Otrokov, Mikhail M., Politano, Antonio, Chulkov, Evgueni V., Arnau Pino, Andrés|||0000-0001-5281-3212, Marinova, Vera|||0000-0002-3499-0212, Das, Pranab K., Fujii, Jun, Vobornik, Ivana, Perfetti, Luca, Mugarza, Aitor|||0000-0002-2698-885X, Goldoni, Andrea|||0000-0001-9989-3889, Marsi, Marino
Tipo de recurso: artículo
Fecha de publicación:2016
País:España
Institución:Universitat Autònoma de Barcelona
Repositorio:Dipòsit Digital de Documents de la UAB
Idioma:inglés
OAI Identifier:oai:ddd.uab.cat:240996
Acceso en línea:https://ddd.uab.cat/record/240996
https://dx.doi.org/urn:doi:10.1021/acs.nanolett.5b02635
Access Level:acceso abierto
Palabra clave:Topological insulator
Phthalocyanine
ARPES
Surface states
Dirac cone
Charge transfer
Descripción
Sumario:Topological insulators are a promising class of materials for applications in the field of spintronics. New perspectives in this field can arise from interfacing metal-organic molecules with the topological insulator spin-momentum locked surface states, which can be perturbed enhancing or suppressing spintronics-relevant properties such as spin coherence. Here we show results from an angle-resolved photemission spectroscopy (ARPES) and scanning tunnelling microscopy (STM) study of the prototypical cobalt phthalocyanine (CoPc)/BiSe interface. We demonstrate that that the hybrid interface can act on the topological protection of the surface and bury the Dirac cone below the first quintuple layer.