Magnetic impurities bridging nanocontacts and break junctions of nearly magnetic metals may lead to permanent moments, analogous to the giant moments well known in the bulk case. A numerical renormalization group (NRG) study shows that, contrary to mean-field–based expectations, a permanent moment never arises within an Anderson model, which invariably leads to strong Kondo screening. In the presence of an additional ferromagnetic intersite exchange coupling between leads and impurity, realistic for nearly ferromagnetic leads, the NRG may instead stabilize a permanent moment. The resulting state is a rotationally invariant spin, which differs profoundly from mean field and whose physical properties are those of a ferromagnetic Kondo model as opposed to the more conventional antiferromagnetic one, where the localized moment gets eventually screened by the conduction electrons. A sign inversion of the zero-bias anomaly and other spectroscopic signatures of the switch from regular to ferromagnetic Kondo are outlined.

Lack of Kondo screening at nanocontacts of nearly magnetic metals / Gentile, P.; De Leo, L.; Fabrizio, M.; Tosatti, E.. - In: EUROPHYSICS LETTERS. - ISSN 0295-5075. - 87:2(2009), pp. 1-5. [10.1209/0295-5075/87/27014]

Lack of Kondo screening at nanocontacts of nearly magnetic metals

Fabrizio, M.;Tosatti, E.
2009-01-01

Abstract

Magnetic impurities bridging nanocontacts and break junctions of nearly magnetic metals may lead to permanent moments, analogous to the giant moments well known in the bulk case. A numerical renormalization group (NRG) study shows that, contrary to mean-field–based expectations, a permanent moment never arises within an Anderson model, which invariably leads to strong Kondo screening. In the presence of an additional ferromagnetic intersite exchange coupling between leads and impurity, realistic for nearly ferromagnetic leads, the NRG may instead stabilize a permanent moment. The resulting state is a rotationally invariant spin, which differs profoundly from mean field and whose physical properties are those of a ferromagnetic Kondo model as opposed to the more conventional antiferromagnetic one, where the localized moment gets eventually screened by the conduction electrons. A sign inversion of the zero-bias anomaly and other spectroscopic signatures of the switch from regular to ferromagnetic Kondo are outlined.
2009
87
2
1
5
27014
Gentile, P.; De Leo, L.; Fabrizio, M.; Tosatti, E.
File in questo prodotto:
File Dimensione Formato  
0902.0254.pdf

non disponibili

Descrizione: preprint
Tipologia: Documento in Pre-print
Licenza: Non specificato
Dimensione 987.46 kB
Formato Adobe PDF
987.46 kB Adobe PDF   Visualizza/Apri   Richiedi una copia

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.11767/14284
Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus 9
  • ???jsp.display-item.citation.isi??? 9
social impact