We report here the first observation of
Na2 Rydberg states with an excited
Na2+ 1 $^{2}\mathrm{\ensuremath{\Pi}}_{\mathit{u}}$ The principle of our experiment is to prepare a Rydberg state associated with the ion in its ground state and then to excite the
Na2+ core with a tunable laser. The autoionization processes occurring in these states as well as the internal energy redistribution of the singly excited Rydberg states are discussed. Finally, the energy levels of the 1 $^{2}\mathrm{\ensuremath{\Pi}}_{\mathrm{u}}$ state of
Na2+ are deduced.
Abstract We present quantum mechanical calculations of autoionization rates for two rubidium Rydberg atoms with weakly overlapping electron clouds. We neglect exchange effects and consider tensor products of independent atom states forming an approximate basis of the two-electron state space. We consider large sets of two-atom states with randomly chosen quantum numbers and find that the charge overlap between the two Rydberg electrons allows one to characterise the magnitude of the autoionization rates. If the electron clouds overlap by more than one percent, the autoionization rates increase approximately exponentially with the charge overlap. This finding is independent of the energy of the initial state.
Measurements of the total yield and rotational distribution of hydrogen molecules formed in chemical reactions or emanating from a surface provide detailed information on the dynamics of these interactions. We have developed a technique which uses a two-photon resonant transition (excited with counterpropagating light beams) to the E electronic state followed by a onephoton transition to the autoionizing continuum of the molecular ion to count different isotopic species in specific rotational levels. To calculate the sensitivity and selectivity of the scheme, we have measured the radiative transition rate, the thermally averaged cross section for elastic scattering to a nearby electronic state, and the real and imaginary parts of the inelastic scattering cross section in the E state. Measurements of the total yield and rotational