We have observed a double-peak structure around 300 cm-1 in the Raman
spectrum of Pb2Sr2NdCu3O8+delta single crystals. Polarization-dependen
t measurements show clearly the B1g symmetry character of both peaks.
Their dependence on temperature, isotopic substitution, and polarizati
on can be interpreted by postulating a coupling between a crystal-fiel
d (CF) excitation of the Nd3+ 4f electrons and the B1g phonon mode. We
have fitted the spectra obtained at different temperatures in Pb2Sr2N
dCu3O8+delta single crystals, and also earlier observations in NdBa2Cu
3O7, with a theoretical model taking the occupation of CF excitations
and phonons into account. From these fits we derive the CF-excitation-
phonon coupling constant V for the two materials, the unperturbed ener
gies of the phonon omega(Ph) and the CF excitation omega(CF), and a pa
rameter kappa, which accounts for the temperature dependence of V. For
NdBa2Cu3O7 the data reveal a self-energy anomaly of the B1g mode near
T(c). We have also estimated the coupling constant V for Pb2Sr2NdCu3O
8 using experimental CF parameters from NdBa2Cu3O6 and structural info
rmation of Pb2Sr2NdCu3O8. We find Absolute value of V = 21.7 cm-1, in
good agreement with the experimental value of (23 +/- 3) cm-1 at 10 K.