Geometry and electronic band structure of surfaces: the case of Ge(111): Sn and C(111) (Articolo in rivista)

Type
Label
  • Geometry and electronic band structure of surfaces: the case of Ge(111): Sn and C(111) (Articolo in rivista) (literal)
Anno
  • 2006-01-01T00:00:00+01:00 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
  • 10.1007/s00339-006-3694-x (literal)
Alternative label
  • Pulci, O1; Marsili, M1; Gori, P2; Palummo, M1; Cricenti, A2; Bechstedt, F3; Del Sole, R1 (2006)
    Geometry and electronic band structure of surfaces: the case of Ge(111): Sn and C(111)
    in Applied physics. A, Materials science & processing (Print)
    (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#autori
  • Pulci, O1; Marsili, M1; Gori, P2; Palummo, M1; Cricenti, A2; Bechstedt, F3; Del Sole, R1 (literal)
Pagina inizio
  • 361 (literal)
Pagina fine
  • 369 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroVolume
  • 85 (literal)
Rivista
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroFascicolo
  • 4 (literal)
Note
  • ISI Web of Science (WOS) (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#affiliazioni
  • 1 European Theoretical Spectroscopy Facility (ETSF) and CNR-INFM, CNISM, Department of Physics, University of Rome 'Tor Vergata', Roma, Italy; 2 CNR, Istituto di Struttura della Materia (ISM), Roma, Italy; 3 European Theoretical Spectroscopy Facility (ETSF) and IFTO, Friedrich Schiller Universität, Jena, Germany (literal)
Titolo
  • Geometry and electronic band structure of surfaces: the case of Ge(111): Sn and C(111) (literal)
Abstract
  • We present an ab initio study of two semiconductor surfaces, the alpha phase of Sn on Ge(111) and the cleavage surface of diamond. The theoretical tools used (density functional theory (DFT) and many-body perturbation theory) are discussed in detail, and the advantages and disadvantages of the two approaches are pointed out. We show that in the case of diamond it is essential to go beyond the DFT single-particle approach, and to introduce quasiparticle effects through the GW approximation. (literal)
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