TY - JOUR
T1 - Electron-spectroscopy and -diffraction study of the conductivity of CVD diamond (0 0 1) 2 × 1 surface
AU - Kono, S.
AU - Takano, T.
AU - Shimomura, M.
AU - Goto, T.
AU - Sato, K.
AU - Abukawa, T.
AU - Tachiki, M.
AU - Kawarada, H.
N1 - Funding Information:
This work is partly supported by the Frontier Carbon Technology project of JFCC through Japan New Diamond Forum.
PY - 2003/4/1
Y1 - 2003/4/1
N2 - A chemical vapor deposition as-grown diamond (001) single-domain 2×1 surface was studied by electron-spectroscopy and electron-diffraction in ultrahigh vacuum (UHV). In order to change the surface conductivity (SC) of the diamond in UHV, three annealing stages were used; without annealing, annealing at 300 °C and annealing at 550 °C. From low energy electron diffraction and X-ray photoelectron spectroscopic (XPS) studies, an existence of SC was suggested for the first two stages of annealing and an absence of SC was suggested for the last stage of annealing. Changes in C KVV Auger electron spectroscopic spectra, C KVV Auger electron diffraction (AED) patterns and C 1s XPS peak positions were noticed between the annealing stages at 300 and 550 °C. These changes are interpreted as such that the state of hydrogen involvement in a subsurface of diamond (001)2×1 changes as SC changes. In particular, the presence of local disorder in diamond configuration in SC subsurface is pointed out from C KVV AED. From C 1s XPS peak shifts, a lower bound for the Fermi-level for SC layers from the valence band top is presented to be ∼0.5 eV.
AB - A chemical vapor deposition as-grown diamond (001) single-domain 2×1 surface was studied by electron-spectroscopy and electron-diffraction in ultrahigh vacuum (UHV). In order to change the surface conductivity (SC) of the diamond in UHV, three annealing stages were used; without annealing, annealing at 300 °C and annealing at 550 °C. From low energy electron diffraction and X-ray photoelectron spectroscopic (XPS) studies, an existence of SC was suggested for the first two stages of annealing and an absence of SC was suggested for the last stage of annealing. Changes in C KVV Auger electron spectroscopic spectra, C KVV Auger electron diffraction (AED) patterns and C 1s XPS peak positions were noticed between the annealing stages at 300 and 550 °C. These changes are interpreted as such that the state of hydrogen involvement in a subsurface of diamond (001)2×1 changes as SC changes. In particular, the presence of local disorder in diamond configuration in SC subsurface is pointed out from C KVV AED. From C 1s XPS peak shifts, a lower bound for the Fermi-level for SC layers from the valence band top is presented to be ∼0.5 eV.
KW - Auger electron diffraction
KW - Auger electron spectroscopy
KW - Chemical vapor deposition
KW - Diamond
KW - Surface electrical transport (Surface conductivity, Surface recombination, etc.)
KW - X-ray photoelectron spectroscopy
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U2 - 10.1016/S0039-6028(03)00241-3
DO - 10.1016/S0039-6028(03)00241-3
M3 - Article
AN - SCOPUS:0037376814
SN - 0039-6028
VL - 529
SP - 180
EP - 188
JO - Surface Science
JF - Surface Science
IS - 1-2
ER -