Real space manifestations of coherent screening in atomic scale Kondo lattices

The interaction among magnetic moments screened by conduction electrons drives quantum phase transitions between magnetically ordered and heavy-fermion ground states. Here, starting from isolated magnetic impurities in the Kondo regime, we investigate the formation of the finite size analogue of a h...

Descripción completa

Detalles Bibliográficos
Autores: Moro Lagares, María, Korytár, Richard, Piantek, Marten, Robles, Roberto|||0000-0001-7808-0395, Lorente, Nicolás, Pascual, Jose I., Ibarra, M. Ricardo, Serrate, David|||0000-0002-3260-9641
Tipo de recurso: artículo
Fecha de publicación:2019
País:España
Institución:Universitat Autònoma de Barcelona
Repositorio:Dipòsit Digital de Documents de la UAB
Idioma:inglés
OAI Identifier:oai:ddd.uab.cat:211662
Acceso en línea:https://ddd.uab.cat/record/211662
https://dx.doi.org/urn:doi:10.1038/s41467-019-10103-5
Access Level:acceso abierto
Palabra clave:Electronic properties and materials
Magnetic properties and materials
Surfaces, interfaces and thin films
Descripción
Sumario:The interaction among magnetic moments screened by conduction electrons drives quantum phase transitions between magnetically ordered and heavy-fermion ground states. Here, starting from isolated magnetic impurities in the Kondo regime, we investigate the formation of the finite size analogue of a heavy Fermi liquid. We build regularly-spaced chains of Co adatoms on a metallic surface by atomic manipulation. Scanning tunneling spectroscopy is used to obtain maps of the Kondo resonance intensity with sub-atomic resolution. For sufficiently small interatomic separation, the spatial distribution of Kondo screening does not coincide with the position of the adatoms. It also develops enhancements at both edges of the chains. Since we can rule out any other interaction between Kondo impurities, this is explained in terms of the indirect hybridization of the Kondo orbitals mediated by a coherent electron gas, the mechanism that causes the emergence of heavy quasiparticles in the thermodynamic limit.