TY - JOUR
T1 - Hard x-ray photoelectron spectroscopy and electrical characterization study of the surface potential in metal/Al2O3/GaAs(100) metal-oxide-semiconductor structures
AU - Walsh, Lee A.
AU - Hughes, Greg
AU - Lin, Jun
AU - Hurley, Paul K.
AU - O'Regan, Terrance P.
AU - Cockayne, Eric
AU - Woicik, Joseph C.
PY - 2013/7/30
Y1 - 2013/7/30
N2 - Hard x-ray photoelectron spectroscopy (HAXPES) has been used to study metal-oxide-semiconductor (MOS) structures fabricated with both high (Ni) and low (Al) work-function metals on 8-nm thick Al2O3 dielectric layers, deposited on sulfur passivated n- and p-doped GaAs substrates. A binding energy difference of 0.6 eV was measured between the GaAs core levels of the n- and p-doped substrates in the absence of gate metals, indicating different Fermi level positions in the band gap. Subsequent photoemission measurements made on the MOS structures with the different work-function metals displayed very limited change in the GaAs core level binding energies, indicating that the movement of the Fermi level at the Al 2O3/GaAs interface is restricted. Using a combination of HAXPES measurements and theoretical calculations, the Fermi level positions in the band gap have been determined to be in the range of 0.4-0.75 eV and 0.8-1.11 eV above the valence band maximum for p- and n-type GaAs, respectively. Analysis of capacitance voltage (C-V) measurements on identically prepared samples yield very similar Fermi level positions at zero applied gate bias. The C-V analysis also indicates a higher interface defect density (Dit) in the upper half of the GaAs bandgap.
AB - Hard x-ray photoelectron spectroscopy (HAXPES) has been used to study metal-oxide-semiconductor (MOS) structures fabricated with both high (Ni) and low (Al) work-function metals on 8-nm thick Al2O3 dielectric layers, deposited on sulfur passivated n- and p-doped GaAs substrates. A binding energy difference of 0.6 eV was measured between the GaAs core levels of the n- and p-doped substrates in the absence of gate metals, indicating different Fermi level positions in the band gap. Subsequent photoemission measurements made on the MOS structures with the different work-function metals displayed very limited change in the GaAs core level binding energies, indicating that the movement of the Fermi level at the Al 2O3/GaAs interface is restricted. Using a combination of HAXPES measurements and theoretical calculations, the Fermi level positions in the band gap have been determined to be in the range of 0.4-0.75 eV and 0.8-1.11 eV above the valence band maximum for p- and n-type GaAs, respectively. Analysis of capacitance voltage (C-V) measurements on identically prepared samples yield very similar Fermi level positions at zero applied gate bias. The C-V analysis also indicates a higher interface defect density (Dit) in the upper half of the GaAs bandgap.
UR - https://www.scopus.com/pages/publications/84883147650
U2 - 10.1103/PhysRevB.88.045322
DO - 10.1103/PhysRevB.88.045322
M3 - Article
AN - SCOPUS:84883147650
SN - 1098-0121
VL - 88
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 4
M1 - 045322
ER -