The electronic structures of hydrogen in SrTiO3 are simulated by the DV-X a
lpha molecular orbital method. In pure SrTiO3, there is a band gap of about
3.5 eV between the O-2p valence band and the Ti-3d conduction band, in agr
eement with experiments. When Sc is doped into SrTiO3, an acceptor level ap
pears just above the valence band. On the other hand, when hydrogen is intr
oduced into SrTiO3, a donor level appears below the conduction band. The mo
lecular orbital of the donor level is composed mostly of the Ti-3d and 0-2p
electrons, but still there is a small occupancy (6% similar to 12%) of the
H-ls electrons in it. When both Sc and hydrogen coexist in SrTiO3, charge
transfer takes place from the donor level to the acceptor level. As a resul
t of this charge compensation, the effective ionicity of hydrogen becomes a
bout + 0.17 similar to + 0.24, the value of which is dependent on the hydro
gen positions in the crystal lattice. Also, the chemical bond strengths bet
ween constituent ions are modified largely by dopants. For example, the Sc
doping tends to strengthen the chemical bond between hydrogen and oxygen io
ns, but instead to weaken the chemical bond between the oxygen ion and the
surrounding metal ions. In addition, it is shown that an oxygen ion vacancy
makes the defect level below the conduction band in the Sc-doped oxide. (C
) 1999 Published by Elsevier Science B.V. All rights reserved.