ABSTRACT

Among the many crystalline lasers based on insulating compounds doped with Ln3+ ions, 1 only one laser is known to generate according to a classical three-level operating scheme, this being the “blue-green” lasing of LiYF4:Pr3+ (its stimulated emission [SE] transition terminates at the lower [zero] Stark level of the ground 3H4 state of Pr3+ ions). 2 For all others the terminal laser level usually has an energy Eterm ≫ kT. In these cases the number of excited Ln3+ ions distributed over the working levels, mainly, the initial laser ones, is small and amounts to a few percent of the total number of generating ions in a crystal. This indicates that SE in those multilevel Ln3+ systems proceeds with practically fully populated levels of the ground state (their usual population is N0 = 1019 to 1021 cm−3, which corresponds to Ln3+ ion concentration amounting to CLn = 0.1 to 10 at.%).