Mcm. Delucas et al., EXCITATION AND EMISSION THERMAL SHIFTS IN ABF(3)MN2- COUPLING WITH IMPURITY VIBRATIONAL-MODES( PEROVSKITES ), Journal of physics. Condensed matter, 7(38), 1995, pp. 7535-7548
The thermal shifts undergone by the first moment of the (6)A(1g)(S) --
> T-4(1g)(G) excitation band and the associated emission band of Mn2+-
doped ABF(3) perovskites are investigated in the 9-300 K temperature r
ange. It is found that these shifts are similar for the whole series a
nd have average values of +150 and +450 cm(-1) for excitation and emis
sion, respectively. Both the sign and the magnitude of these different
thermal shifts are explained in terms of (i) the phonon assistance me
chanism required to gain intensity of the parity-forbidden transitions
, (ii) the quadratic electron-phonon coupling and (iii) thermal expans
ion effects. To achieve this analysis a previous discussion upon the n
ature of the vibrational modes seen in the optical spectra is carried
out. It is stressed that the impurity vibrational mode displaying HBAR
omega(g) = 570 cm(-1) in the emission spectrum of KMgF3:Mn2+ exhibits
a value of 540 cm(-1) in the corresponding excitation spectrum. This
situation, which is also found for other modes seen in the optical spe
ctra of KMgF3:Mn2+, indicates that the mode (though associated with th
e LO(3) branch of KMgF3) is not a pure mode of the lattice but display
s a kind of resonant character. As a salient feature the calculated th
ermal shifts are based on the experimental shifts experienced by the f
requencies of the optical and acoustic modes on going from the ground
(6)A(1g) to the excited T-4(1g) state of MnF64-. At variance with find
ings for the R lines in Cr3+ and V2+, it is clearly demonstrated that
the explicit and implicit contributions to the thermal shift of the ze
ro-phonon line in MnF64- are similar and both induce red shifts upon h
eating. Moreover the present analysis reveals that the explicit contri
bution to the thermal shift undergone by the zero-phonon line of KMgF3
:Mn2+ is mainly dominated by the odd-parity low-energy modes. The calc
ulated thermal shifts reproduce reasonably well the experimental data.