A polar LiNbO3 (LN)-type oxide LiSbO3 was
synthesized by a high-temperature heat treatment under a pressure
of 7.7 GPa and found to exhibit ferroelectricity. The crystal structural
refinement using the data of synchrotron powder X-ray diffraction
and neutron diffraction and the electronic structure calculation of
LN-type LiSbO3 suggest a covalent-bonding character between
Sb and O. When comparing the distortion of BO6 in LN-type
ABO3, the distortions of SbO6 in LiSbO3 and SnO6 in ZnSnO3, which included a B cation
with a d10 electronic configuration, were smaller than
those of BO6 in LN-type oxides having the second-order
Jahn–Teller active B cation, e.g., LiNbO3 and ZnTiO3. The temperature dependence of the lattice parameters, second
harmonic generation, dielectric permittivity, and differential scanning
calorimetry made it clear that a second-order ferroelectric–paraelectric
phase transition occurs at a Curie temperature of T
c = 605 ± 10 K in LN-type LiSbO3. Further,
first-principles density functional theory calculation suggested that
perovskite-type LiSbO3 is less stable than LN-type LiSbO3 under even high pressure, and the ambient phase of LiSbO3 directly transforms to LN-type LiSbO3 under high
pressure. The phase stability of LN-type LiSbO3 and the
polar and ferroelectric properties are rationalized by the covalent
bonding of Sb–O and the relatively weak Coulomb repulsion between
Li+ and Sb5+.