“…For superradiance in the ensemble of two level atoms, the account for the effects of local field gives rise to a dynamic shift of the resonant fre quency depending on the difference of populations between the levels [1], while, for the ensemble of three level atoms with the scheme of the transi tions, the dynamic frequency shifts induced by the local field give rise to competition of transitions in the high frequency channels and lead to a coherent Raman transition between sublevels of the lower dou blet [10,11]. Specifically, for collective spontaneous emission (superradiance) to be possible in an ensem ble of two level atoms, the initial population inversion in the operating transition is needed [12][13][14][15][16], while, for three level media, there exists a possibility of inver sionless superradiance [17][18][19][20][21][22][23][24], with the initial popu lation of the upper levels being smaller than one half:…”