The oscillator strengths and relative vibronic intensity distribution
of the (F-2(5/2))Gamma(8), Gamma(7)<--Gamma(6)(F-2(7/2)) transitions o
f the YbCl63- complex ion at an octahedral symmetry site in the Cs2NaY
bCl6 lattice have been measured experimentally and calculated using a
combined vibronic crystal-field-ligand polarization approach. The vibr
onic crystal-field contribution to the total transition dipole moment
of the various excitations was worked out both with and without invoki
ng closure over the central metal ion intermediate electronic stares a
nd the intensity was assumed to be derived from both a parity and a sp
in-allowed d<--f transition with the cooperation of the odd-parity vib
rational modes of the complex ion. Quadrupole and hexadecapole terms h
ave bern included in the ligand polarization contribution. Attention h
as been given to the correct choice of phases for both the electronic
and the vibrational wave functions in order to ensure the right sign f
or the cross term which couples together the crystal field and the lig
and polarization transition dipole vectors, The an initio formalism em
ployed avoids the use of any adjustable parameters in calculating the
vibronic intensities. The calculated oscillator strengths of vibronic
transitions are within order of magnitude agreement with experimental
values. The sensitivity of the calculated values to the use of differe
nt force fields has been investigated. The experimentally measured tot
al oscillator strengths for the (F-2(5/2))Gamma(8), Gamma(7)<--Gamma(6
)(F-2(7/2)) transitions of YbCl63- diluted into the transparent Cs2NaG
dCl6 host remain constant with change in Yb3- concentration although d
eviation of the chromophore from octahedral symmetry is evident at int
ermediate concentrations, A comparison with the vibronic sidebands of
Cs2LiYbCl6 and Cs2KYbF6 is made.