S. Lopezmoraza et Z. Barandiaran, EXCITED-STATE ABSORPTION-SPECTRA OF V2-DOPED FLUOROPEROVSKITES - AN AB-INITIO MODEL POTENTIAL EMBEDDED-CLUSTER STUDY(), The Journal of chemical physics, 105(1), 1996, pp. 50-61
In this paper we present an ab initio model potential embedded-cluster
study of the electronic structure of the local excited states of V2+-
doped KMgF3, KZnF3, and CsCaF3 fluoroperovskites, which are more direc
tly involved in their potential laser activity: the T-4(2g), T-4(1g)a,
and T-4(1g)b, states of the (VF6)(4-) embedded-cluster. The ab initio
model potential embedded-cluster model used allows for the considerat
ion of intracluster electron correlation and Jahn-Teller coupling in t
he excited states, as well as of lattice effects which include quantum
mechanical interactions resulting from a relaxed, dipole polarized cr
ystal lattice. The embedding potentials enable the geometry optimizati
on of the embedded-cluster electronic ground-state but also of the exc
ited states; as a consequence, the ab initio calculation of the vertic
al ground-state absorption, excited-state absorption, and emission spe
ctra is possible and it is done in this work, without resorting to the
use of experimental structural parameters of the local defect, which,
in any case, are not available for the ground state and not attainabl
e for the excited states. The agreement of the calculated ground-state
absorption, excited-state absorption, and emission transition energie
s with the available experimental data is satisfactory and systematic.
Our results allow for the discussion of (a) the competition between t
he infrared T-4(2g)-->T-4(1g)a, excited-state absorption and the T-4(2
g)-->(4)A(2g) spontaneous emission, (b) the overlap between the excite
d-state absorption bands and the pumping bands, and (c) the (4)A(2g)--
>T-4(2g) reabsorption, for all three V2+-doped fluoroperovskites, as w
ell as their host dependency. The overall conclusion is that the laser
efficiency is expected to deteriorate in the investigated series, goi
ng from KMgF3:V2+ to CsCaF3:V2+. (C) 1996 American Institute of Physic
s.