S. Steinsvik et al., THE DEFECT STRUCTURE OF SRTI1-XFEXO3-Y (X=0-0.8) INVESTIGATED BY ELECTRICAL-CONDUCTIVITY MEASUREMENTS AND ELECTRON-ENERGY-LOSS SPECTROSCOPY(EELS), Journal of physics and chemistry of solids, 58(6), 1997, pp. 969-976
The electrical properties and defect structure of selected composition
s in the SrTi1-xFexO3-y system (x = 0-0.8) have been studied using van
der Pauw 4-point conductivity measurements and electron energy loss s
pectroscopy (EELS). Using X-ray powder diffraction and selected area e
lectron diffraction (SAD), the basic crystal structure was determined
to be cubic perovskite for all the investigated compositions. A supers
tructure cell 2.2.1 times the ordinary perovskite cell was found in ma
terials with x = 0.6 and x = 0.8. The conductivity was measured on sin
tered tablets as a function of the partial pressure of oxygen (pO(2) =
10(-25) to 1 atm) at 600-1100 degrees C. The materials investigated a
re predominantly p-type electronic conductors at high, n-type conducto
rs at low, and ionic conductors at intermediate oxygen partial pressur
es. All conductivity contributions increase with increasing iron conte
nt. This can be attributed to the acceptor role of the iron, decreased
band gap and decreased activation energy for oxygen vacancy migration
. The EELS spectra show a shoulder below the oxygen K-edge, increasing
in magnitude with increasing iron content and oxygen partial pressure
. This shoulder is assigned to empty electron energy states at some of
the oxygen atoms, indicating that electron holes are associated with
lattice oxygen in the structure. Spectra from the Fe L-edge showed sma
ll changes, suggesting that there are few or no empty states at the ir
on atoms. (C) 1997 Elsevier Science Ltd.