“…Unfortunately, an uncertainty in parameters of superexchange interaction, particularly in the Mott-Hubbard value U from one side, and in the JT energy ∆ from the other side, is still a challenge for theoreticians and it is not yet clear where the orbitons should be looked for in measurements. In a limit of weak JT coupling, the orbital excitations in LaMnO 3 are predicted to appear around 1600 cm −1 (0.2 eV), as a result of the superexchange interaction [14,15], which indicates on the feature, observed in the second-order Raman scattering experiment in the 900-1400 cm −1 (0.11-0.17 eV) range [8]. If the contributions from SE and JT effects are considered on equal footing, the elementary excitations of the system, according to the theory predictions, are mixed modes with both phonon and orbital character, and the phonon-orbital excitations appear as Franck-Condon sidebands at energy intervals of the Jahn-Teller vibrational energy [16].…”