Absolute differential cross sections of non-characteristic radiation emitted in energetic heavy-ion collisions (Ep = 3.92-48 MeV, Z = I 1-22) can only be explained in the framework of quasimolecular radiation. All other processes, particularly bremsstrahlung mechanisms are found to be negligible. For high projectile and photon energies the one-step quasimolecular radiation is dominant in solid targets, whereas the two-step process contributes mainly at low projectile and photon energies.The non-characteristic radiation (NCR) above the K-lines emitted in energetic heavy-ion collisions has been the subject of several investigations [1][2][3][4][5][6][7][8] during the last years. For adiabatic collisions (vp ~ v~, where vp and v~ are the projectile and the K-shell electron velocities, respectively) various experimental results [1][2][3][4] were interpreted in the framework of quasimolecular radiation (MOR). In this process the vacancy in the lsa quasimolecular orbital (MO) can be produced either in the K-shell of the projectile in a previous collision (two-step MOR(MOR II)) or in the same collision (one-step MOR(MOR I)), where the vacancy decays. In less adiabatic collisions (Vp