Raman-scattering experiments have been carried out on polycrystalline sampl
es of La0.65Ca0.35Mn O-16(3) and isotope-exchanged La0.65Ca0.35Mn O-18(3) a
s a function of temperature. The most interesting feature in the spectra. i
s a vibrational mode that occurs at a nominal frequency of omega(0) approxi
mate to 230 cm(-1), which is assigned to an out-of-phase rotational mode th
at involves motion of the O(1) atoms. The frequency of this phonon depends
strongly on the Ca concentration and has been correlated with the strength
of the Jahn-Teller lattice distortion as measured by the tolerance factor.
As the temperature is lowered through the critical temperature, the phonon
frequency omega(0) increases rather abruptly and continues to harden as the
temperature is lowered further. In contrast, the linewidth Gamma(0) decrea
ses abruptly when the sample passes through the transition from the paramag
netic insulating phase to the more metallic ferromagnetic phase. The observ
ed temperature dependences of the frequency and linewidth are well describe
d by a model that incorporates a double-exchange mechanism in the presence
of an electron-phonon interaction. The agreement between experiment and the
ory suggests that the temperature dependence of the phonon is determined pr
imarily by the spin alignment associated with the double-exchange mechanism
. The results for both omega(0) and Gamma(0) imply that there are no signif
icant structural modifications associated with the transition to the ferrom
agnetic phase. Finally, the linewidth Gamma(0) in the isotope-exchanged sam
ple (O-18) is Smaller than in the O-16 sample, an observation that is consi
stent with the smaller electron-phonon-coupling constant in the O-18 compou
nd. [S0163-1829(99)06413-9].