The structural geometry, vibrations and deformation density Delta rho
for lithium niobate, LSTbO3, and Lithium tantalate, LiTaO3, are derive
d from synchrotron radiation diffraction measurements. Electron densit
y is transferred from the Nb (Ta) atom towards the large O-3 triangle
near the Li atom. Spontaneous polarizations of 0.43 (LibNbO(3)) and 0.
33 cm(-2) (LiTaO3), calculated with Hirshfeld charges, agree qualitati
vely with experimental values of 0.71 and 0.50 cm(-2), respectively. B
oth strong Li ... Nb (Ta) interactions in the structure are markedly s
horter than all Li ... Li, Nb ... Nb or Ta ... Ta vectors, as expected
if the Li and Nb (Ta) cations carry charges of opposite sign. The Li
atom's negative charge plays a pivotal role in the polarization respon
sible for ferroelectricity. LiNbO3, space group R3c, rhombohedral, M-r
= 147.8, a = 5.493 (2) Angstrom, alpha = 55.89 (3)degrees, V = 106.02
(4) Angstrom(3), Z = 2, D-x = 4.629 Mg m(-3), F(000) = 136, mu(0.7 An
gstrom) = 5.01 mm(-1), gamma(min) = 0.27, T = 293 K, R = 0.015, wR = 0
.015, S = 3.276 (84) for 773 unique reflections. LiTaO3, R3c, rhombohe
dral, M-r = 235.9, a = 5.471 (2) Angstrom, alpha = 56.16 (3)degrees, V
= 105.51 (4) Angstrom(3), Z = 2, D-x = 7.412 Mg m(-3), F(000) = 200,
mu(0.7 Angstrom) = 50.03 mm(-1), gamma(min) = 0.32, T = 293 K, R = 0.0
16, wR = 0.022, S = 1.372 (35) for 773 unique reflections.