Crystals of cubic Sc2O3, LU2O3, Yb2O3 and Dy2O3 were grown as single-crysta
l fibres of dimensions of similar to0.5 mm x 15 mm using the laser-heated p
edestal growth technique. Refractive indices of prisms prepared from these
fibres were measured at wavelengths of 435.8-643.8 nm and were used to calc
ulate n at lambda = 589.3 nm (n(D)) and at lambda = infinity (n(infinity))
using the one-term Sellmeier equation 1(n(2) - 1) = -A/lambda (2) + B. In a
ddition, using the dispersion of two refractive indices of a larger crystal
of monoclinic Gd2O3:Nd, we have estimated mean values of (n(infinity)) and
(n(D)). Total polarizabilities, alpha (total) were calculated from n(infin
ity) and the Lorenz-Lorentz equation. Refractive indices, no, and dispersio
n values, A, were, respectively, 1.9943 and 66 for Sc2O3, 1.9349 and 66 for
LU2O3, 1.9470 and 68 for Yb2O3, 1.9757 and 73 for DY2O3 and (2.086) and 62
x 10(-16) m(2) for Gd2O3:Nd. These data were used to estimate the refracti
ve indices and total polarizabilities of cubic Tm2O3, Er2O3, Ho2O3, Tb2O3,
Gd2O3 and Eu2O3, monoclinic Sm2O3 and hexagonal Nd2O3 from plots of the typ
e alpha (total) = a (atomic number) + b.