Your browser doesn't support javascript.
loading
Charge transfer doping of silicon.
Rietwyk, K J; Smets, Y; Bashouti, M; Christiansen, S H; Schenk, A; Tadich, A; Edmonds, M T; Ristein, J; Ley, L; Pakes, C I.
Afiliación
  • Rietwyk KJ; Department of Physics, La Trobe University, Victoria 3086, Australia.
  • Smets Y; Department of Physics, La Trobe University, Victoria 3086, Australia.
  • Bashouti M; Max-Planck-Institute for the Science of Light, D-91058 Erlangen, Germany and Institute of Nanoarchitectures for solar energy conversion, Helmholtz-Centre Berlin (HZB), D-14109 Berlin, Germany.
  • Christiansen SH; Institute of Nanoarchitectures for solar energy conversion, Helmholtz-Centre Berlin (HZB), D-14109 Berlin, Germany.
  • Schenk A; Department of Physics, La Trobe University, Victoria 3086, Australia.
  • Tadich A; Australian Synchrotron, 800 Blackburn Road, Clayton, Victoria 3168, Australia.
  • Edmonds MT; School of Physics, Monash University, Clayton, Victoria 3800, Australia.
  • Ristein J; Technische Physik, Universität Erlangen, D-91058 Erlangen, Germany.
  • Ley L; Department of Physics, La Trobe University, Victoria 3086, Australia and Technische Physik, Universität Erlangen, D-91058 Erlangen, Germany.
  • Pakes CI; Department of Physics, La Trobe University, Victoria 3086, Australia.
Phys Rev Lett ; 112(15): 155502, 2014 Apr 18.
Article en En | MEDLINE | ID: mdl-24785050
ABSTRACT
We demonstrate a novel doping mechanism of silicon, namely n-type transfer doping by adsorbed organic cobaltocene (CoCp2*) molecules. The amount of transferred charge as a function of coverage is monitored by following the ensuing band bending via surface sensitive core-level photoelectron spectroscopy. The concomitant loss of electrons in the CoCp2* adlayer is quantified by the relative intensities of chemically shifted Co2p components in core-level photoelectron spectroscopy which correspond to charged and neutral molecules. Using a previously developed model for transfer doping, the evolution in relative intensities of the two components as a function of coverage has been reproduced successfully. A single, molecule-specific parameter, the negative donor energy of -(0.50±0.15) eV suffices to describe the self-limiting doping process with a maximum areal density of transferred electrons of 2×1013 cm-2 in agreement with the measured downward band bending. The advantage of this doping mechanism over conventional doping for nanostructures is addressed.
Buscar en Google
Banco de datos: MEDLINE Idioma: En Año: 2014 Tipo del documento: Article
Buscar en Google
Banco de datos: MEDLINE Idioma: En Año: 2014 Tipo del documento: Article