“…As shown in the recent review [1], the experimental evidences of a super-fluorescence (collective spontaneous emission under a pulsed pumping) give prospects for the creation of the superradiant heterolasers with continuous-wave (CW) incoherent pumping. As is well-known, in this class of lasers, the superradiance condition reads ″ 0 > −1 2 , where ″ 0 ≈̄2 − 1/ 2 − 1/ * 2 is the growth rate of the most unstable hot mode, = √2 2 21 0 Γ/( 0 ℏ) the cooperative frequency,̄the population inversion (normalized to unity) of the active centers averaged over a cavity, 0 their density, a photon lifetime for a given cavity mode, Γ the mode-filling factor, 0 the dielectric (real) permittivity of a background medium (matrix), 21 the central frequency of a spectral line of active centers, their dipole transition moment, 2/ 2 and 2/ * 2 the homogeneous and inhomogeneous line broadening (see also [2,3]).…”