| Abstract
| - New oxides, BiAlO3 and BiGaO3, were prepared using high-temperature and high-pressure (6 GPa) technique. BiAlO3 is a perovskite-type oxide isotypic with multiferroic BiFeO3 and, therefore, possesses a spontaneous polarization. BiGaO3 is a pyroxene-type oxide having infinite chains of corner-shared GaO4 tetrahedra. In solid solutions of BiAl1-xGaxO3, a phase structurally related to PbTiO3 was found.
- New oxides, BiAlO3 and BiGaO3, were prepared using a high-pressure high-temperature technique at6 GPa and 1273−1473 K. BiAlO3 is isotypic with multiferroic perovskite-like BiFeO3 and has octahedrallycoordinated Al3+ ions. Structure parameters of BiAlO3 were refined from laboratory X-ray powderdiffraction data (space group R3c; Z = 6; a = 5.37546(5) Å and c = 13.3933(1) Å). BiGaO3 has thestructure closely related to pyroxene-like KVO3. Structure parameters of BiGaO3 were refined from time-of-flight neutron powder diffraction data (space group Pcca; Z = 4; a = 5.4162(2) Å, b = 5.1335(3) Å,and c = 9.9369(5) Å). The GaO4 tetrahedra in BiGaO3 are joined by corners forming infinite (GaO3)3-chains along the a axis. Bi3+ ions in BiGaO3 have 6-fold coordination. Both BiAlO3 and BiGaO3 decomposeat ambient pressure on heating above 820 K to give Bi2M4O9 and Bi25MO39 (M = Al and Ga). Vibrationalproperties of BiAlO3 and BiGaO3 were studied by Raman spectroscopy. In solid solutions of BiAl1-xGaxO3,a C-centered monoclinic phase structurally related to PbTiO3 with lattice parameters of a = 5.1917(4)Å, b = 5.1783(4) Å, c = 4.4937(3) Å, and β = 91.853(3)° was found.
|
