Berlin 2005 – wissenschaftliches Programm
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MO: Molekülphysik
MO 42: Poster II
MO 42.16: Poster
Dienstag, 8. März 2005, 14:00–16:00, Poster HU
Autoionization and double autoionization of the vibrationally selective excited N2(1s−1πg*)(v′)-resonances investigated by dispersed fluorescence spectroscopy (135nm≤ λFl ≤185nm) — •L Werner1, S Lucht1, S Klumpp1, H Schmoranzer1, A Ehresmann1, Ph V Demekhin2, B M Lagutin2, I V Petrov2, V L Sukhorukov2, S Mickat3, R Schill3, and K-H Schartner3 — 1FB Physik, TU Kaiserslautern, D-67653 Kaiserslautern, Germany — 2Rostov State University of Transport Communications, 344038 Rostov-on-Don, Russia — 3I Physikalisches Institut, Justus-Liebig-Universität, D-35392 Gießen, Germany
Synchrotron radiation from the storage ring BESSY II has been used for the vibrationally selective inner-shell photoexcitation of the N2(1s−1πg*)(v′)-resonances using a bandwidth of 75meV at 400eV. The subsequent (double) autoionization into different vibrational levels of the N2+ C 2Σu+ electronic state and into the N22+D 1Σu+ state were investigated using photon-induced fluorescence spectroscopy (PIFS) by measuring the intensities of N2+C−X and N22+D−X bands using a 1m normal incidence monochromator (135nm≤ λFl≤185nm). Simultaneously to the dispersed fluorescence intensities the photoabsorption and the photoion signal were measured. Intensities of the N2+C−X and N22+D−X-bands were measured as a function of the exciting-photon energy. The observed fluorescence intensities are interpreted using calculated Franck-Condon factors for the transition N2X−N2 π*(excitation), N2 π*−N2+C(autoionization) [or alternativly N2 π*−N22+D(double autoioization)] and N2+C−N2+X [or N22+D−N22+X].