Abstract
Radiatsive autoionization (RA) is a spontaneous decay mechanism of highly excited states, whereby the atom or molecule makes a radiative bound- (or quasi-bound-) free transition, emitting a photon and an electron at the same time. Calculations show that, for each transition, the intensity of the emitted radiation peaks on the short-wavelength side. Since RA involves a final empty state, population inversion is achieved once the initial state is populated. The basic lasing condition can thus be satisfied automatically. The phenomenon is analogous to the radiative dissociation process which is the physical mechanism for the excimer laser. Examples are given for the H- and He 2p23p, He- and Li 2p34S0, Li and Be+ 1s2p22p, He 2p3p1P, and 2p3d1D0, as well as for the Li 1s2s2p4P0state which undergoes relativistic RA.