Si oxidation promoted by a platinum (Pt) overlayer has been investigat
ed using x-ray photoelectron spectroscopy and synchrotron radiation ul
traviolet photoelectron spectroscopy. Heat treatments of the specimens
with (similar to 5-nm-Pt/0.5-1-nm-chemical oxide/Si(100)) structure a
t 300-400 degrees C increase the oxide thickness to 4-5 nm. The amount
s of the suboxide species, a(Si+), a(Si2+), and a(Si3+), in the chemic
al oxide layers formed in hydrochloric acid (HCl) plus hydrogen peroxi
de (H2O2) are in the order of a(Si+)>a(Si2+)>a(Si3+), while those for
the oxide layers formed in nitric acid (HNO3) have an order of a(Si3+)
>a(Si2+)approximate to a(Si+). The amounts of the suboxide species in
the former oxide layers are much higher than those in the latter oxide
layers. These results indicate that the HNO3 oxide layers are more hi
ghly oxidized, probably resulting in a higher atomic density and a low
er defect density. Although the initial chemical oxide layers formed i
n HCl+H2O2 are thinner than those grown in HNO3, the former oxide laye
rs become thicker than the latter after the Pt deposition and the heat
treatments below 200 degrees C. This result is attributed to the lowe
r atomic density and the higher defect density of the chemical oxide l
ayers produced in HCl+H2O2, which enhance the diffusion of oxidizing s
pecies. It is suggested that the variation in the atomic density of th
e chemical oxide layers cause the different energy distribution of int
erface states in the Si band gap. (C) 1997 American Institute of Physi
cs.