Electronic structure of the (1×1) oxygen overlayer on TiC(111): Angle-resolved photoemission study
1992; American Physical Society; Volume: 46; Issue: 11 Linguagem: Inglês
10.1103/physrevb.46.7127
ISSN1095-3795
AutoresKazuyuki Edamoto, Atsushi Mochida, Toshihisa Anazawa, Tokio Itakura, Eizo Miyazaki, Hiroo Kato, Shigeki Otani,
Tópico(s)Advanced Chemical Physics Studies
ResumoAngle-resolved photoemission spectroscopy with synchrotron radiation has been used to study the electronic state of oxygen adsorbed on a TiC(111) surface at room temperature. Oxygen is adsorbed dissociatively forming a (1\ifmmode\times\else\texttimes\fi{}1) overlayer on the TiC(111) surface at saturation coverage. The band structure of the (1\ifmmode\times\else\texttimes\fi{}1)-O overlayer is measured in the two symmetry directions; 〈21\ifmmode\bar\else\textasciimacron\fi{} 1\ifmmode\bar\else\textasciimacron\fi{}〉(\ensuremath{\Gamma}\ifmmode\bar\else\textasciimacron\fi{} M\ifmmode\bar\else\textasciimacron\fi{}) and 〈011\ifmmode\bar\else\textasciimacron\fi{}〉(\ensuremath{\Gamma}\ifmmode\bar\else\textasciimacron\fi{} K\ifmmode\bar\else\textasciimacron\fi{}) of the TiC(111) surface. The binding energy of the O 2${\mathit{p}}_{\mathit{z}}$-derived band is always lower than those of the O 2${\mathit{p}}_{\mathit{x}}$- and O 2${\mathit{p}}_{\mathit{y}}$-derived bands throughout the surface Brillouin zone, indicating that the 2${\mathit{p}}_{\mathit{x}}$ and 2${\mathit{p}}_{\mathit{y}}$ orbitals are more important for the chemisorption bond formation.
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