The weak, polarized Raman band assigned to the nu(1) CdO6 mode of the hexaq
uo-Cd(II) ion (T-h symmetry) has been studied over the temperature range fr
om 25 degrees C to 152 degrees C. The isotropic scattering geometry in R-fo
rmat was employed in order to measure the true vibrational contribution of
the band and account for the Boltzmann temperature factor B. The band profi
le as a function of temperature has been examined analytically to extract t
he parameters: position of band maximum, full width at half height (FWHH),
integral intensity of the band and relative molar scattering coefficient, S
-h over the temperature range measured. The dependence on concentration has
also been measured. The 358 cm(-1) band of hexaquo-Cd(II) shifts only 3 cm
(-1) to lower frequencies and broadens about 32 cm(-1) for a 127 degrees C
temperature increase. Two depolarized modes at 235 cm(-1) and 185 cm(-1) co
uld be assigned to nu(2)(e(g)) and nu(5)(f(2g)), respectively. The Raman sp
ectroscopic data suggest that the hexaquo-Cd(II) ion is stable in perchlora
te solution over the temperature range measured. These findings are in cont
rast to CdSO4 solutions, recently measured by one of us, where sulfate repl
aces a water molecule of the first hydration sphere. Ab initio geometry opt
imizations of [Cd(OH2)(6)(2+)] were carried out at the Hartree-Fock and sec
ond order Moller-Plesset levels of theory, using various basis sets up to 6
-31+G*. The vibrational frequencies of the [Cd(OH)(6)(2+)] cation were also
calculated. Scaling the Hartree-Fock vibrational frequencies (HF/6-31G* an
d HF/6-31+G* level) reproduced the measured frequencies of the CdO6 unit. T
he theoretical binding energy for the hexaquo-Cd(II) ion was calculated and
accounts for 66% of the experimental hydration enthalpy of Cd(II). The imp
ortance of the second hydration sphere is also discussed.