The vibrational properties of strongly coupled one-dimensional electron-lattice systems are dis-tinct form those of weakly coupled ones. While the weakly coupled systems have only four localized modes around the soliton and there is overlap between acoustic and optical phonon branches, the strongly coupled systems can possess more localized modes, and no overlap exists. In terms of the coupling constant λ, the boundary beween strong and weak coupling is λe=0.2119. The number of localized modes depends on λ, and each localized mode can only exist for a certain region of λ. Then the whole rane [0.2/π] of λ can be divided into seven regions, each of which has a charac-teristic disposition of the localized modes.