Pa. Tanner et Yl. Liu, RAMAN, ELECTRONIC RAMAN, INFRARED-ABSORPTION AND VISIBLE LUMINESCENCESPECTRUM OF CS2NAEUCL6, Journal of alloys and compounds, 204(1-2), 1994, pp. 93-100
The 457.9 nm and 514.5 nm laser excited spectra of polycrystalline Cs2
NaEuCl6, at room temperature and 120 K are reported. The spectra are i
nterpreted in terms of: (a) Raman transitions involving fundamental mo
des of the EuCl63- moiety, with some features exhibiting different rel
ative intensity as a function of excitation line; (b) Raman transition
s involving lattice modes and combination bands with the phase transit
ion soft mode; (c) electronic Raman bands of Eu3+; and (d) luminescenc
e bands from the electronic and/or vibronic levels of (5D2)GAMMA3,GAMM
A5, (5D1)GAMMA4 and (5D0)GAMMA1 to the electronic and/or vibronic leve
ls of 7F(J) (J=0-6). The 120 K and 10 K infrared absorption spectra Of
CS2NaEuCl6 are reported, and assigned in detail to the transitions in
volving terminal crystal field and/or vibronic levels of 7F(J) (J=2-6)
. A complete interpretation is given for the vibronic structure of the
transitions. Together with the electronic Raman and luminescence resu
lts, all of the energy levels of Eu3+ in Cs2NaEuCl6 up to 21 500 cm-1
have been assigned. At 120 K, the effects of the phase transition are
not apparent from the moiety modes Of CS2NaEuCl6, but the caesium tran
slational mode in the Raman spectrum is split. The degenerate electron
ic levels exhibit splittings of up to several wavenumbers. A compariso
n is made with the corresponding spectra of Cs2LiEuCl6, and a vibratio
nal analysis is given for both compounds. The principal stretching for
ce constant is about 10% greater in Cs2NaEuCl6 than in CS2LiEuCl6, whe
reas the principal bending force constant is about 30% smaller.