{"intvolume":"        39","volume":39,"date_created":"2018-12-11T11:55:57Z","publist_id":"4882","year":"2006","publisher":"IOP Publishing Ltd.","quality_controlled":0,"title":"Studying the N+2(C2Σ+u → X2Σ+g) fluorescence excited via the 1s−1π* resonance","status":"public","type":"journal_article","publication":"Journal of Physics B: Atomic, Molecular and Optical Physics","day":"28","author":[{"full_name":"Ehresmann, Arno","last_name":"Ehresmann","first_name":"Arno"},{"last_name":"Werner","first_name":"Lutz","full_name":"Werner, Lutz"},{"full_name":"Klumpp, Stefan","last_name":"Klumpp","first_name":"Stefan"},{"first_name":"S","last_name":"Lucht","full_name":"Lucht, S"},{"full_name":"Schmoranzer, Hans P","last_name":"Schmoranzer","first_name":"Hans"},{"first_name":"Sascha","last_name":"Mickat","full_name":"Mickat, Sascha"},{"full_name":"Schill, Rüdiger H","last_name":"Schill","first_name":"Rüdiger"},{"last_name":"Schartner","first_name":"Karl","full_name":"Schartner, Karl H"},{"last_name":"Demekhin","first_name":"Philipp","full_name":"Demekhin, Philipp"},{"full_name":"Mikhail Lemeshko","id":"37CB05FA-F248-11E8-B48F-1D18A9856A87","first_name":"Mikhail","last_name":"Lemeshko","orcid":"0000-0002-6990-7802"},{"last_name":"Sukhorukov","first_name":"Victor","full_name":"Sukhorukov, Victor L"}],"page":"283 - 304","doi":"10.1088/0953-4075/39/2/006","month":"01","date_updated":"2021-01-12T06:55:34Z","publication_status":"published","extern":1,"citation":{"short":"A. Ehresmann, L. Werner, S. Klumpp, S. Lucht, H. Schmoranzer, S. Mickat, R. Schill, K. Schartner, P. Demekhin, M. Lemeshko, V. Sukhorukov, Journal of Physics B: Atomic, Molecular and Optical Physics 39 (2006) 283–304.","apa":"Ehresmann, A., Werner, L., Klumpp, S., Lucht, S., Schmoranzer, H., Mickat, S., … Sukhorukov, V. (2006). Studying the N+2(C2Σ+u → X2Σ+g) fluorescence excited via the 1s−1π* resonance. <i>Journal of Physics B: Atomic, Molecular and Optical Physics</i>. IOP Publishing Ltd. <a href=\"https://doi.org/10.1088/0953-4075/39/2/006\">https://doi.org/10.1088/0953-4075/39/2/006</a>","ista":"Ehresmann A, Werner L, Klumpp S, Lucht S, Schmoranzer H, Mickat S, Schill R, Schartner K, Demekhin P, Lemeshko M, Sukhorukov V. 2006. Studying the N+2(C2Σ+u → X2Σ+g) fluorescence excited via the 1s−1π* resonance. Journal of Physics B: Atomic, Molecular and Optical Physics. 39(2), 283–304.","chicago":"Ehresmann, Arno, Lutz Werner, Stefan Klumpp, S Lucht, Hans Schmoranzer, Sascha Mickat, Rüdiger Schill, et al. “Studying the N+2(C2Σ+u → X2Σ+g) Fluorescence Excited via the 1s−1π* Resonance.” <i>Journal of Physics B: Atomic, Molecular and Optical Physics</i>. IOP Publishing Ltd., 2006. <a href=\"https://doi.org/10.1088/0953-4075/39/2/006\">https://doi.org/10.1088/0953-4075/39/2/006</a>.","ama":"Ehresmann A, Werner L, Klumpp S, et al. Studying the N+2(C2Σ+u → X2Σ+g) fluorescence excited via the 1s−1π* resonance. <i>Journal of Physics B: Atomic, Molecular and Optical Physics</i>. 2006;39(2):283-304. doi:<a href=\"https://doi.org/10.1088/0953-4075/39/2/006\">10.1088/0953-4075/39/2/006</a>","ieee":"A. Ehresmann <i>et al.</i>, “Studying the N+2(C2Σ+u → X2Σ+g) fluorescence excited via the 1s−1π* resonance,” <i>Journal of Physics B: Atomic, Molecular and Optical Physics</i>, vol. 39, no. 2. IOP Publishing Ltd., pp. 283–304, 2006.","mla":"Ehresmann, Arno, et al. “Studying the N+2(C2Σ+u → X2Σ+g) Fluorescence Excited via the 1s−1π* Resonance.” <i>Journal of Physics B: Atomic, Molecular and Optical Physics</i>, vol. 39, no. 2, IOP Publishing Ltd., 2006, pp. 283–304, doi:<a href=\"https://doi.org/10.1088/0953-4075/39/2/006\">10.1088/0953-4075/39/2/006</a>."},"date_published":"2006-01-28T00:00:00Z","issue":"2","_id":"2142","abstract":[{"lang":"eng","text":"Fluorescence from fragments formed after the de-excitation of the N*2(1s−1π*) resonance has been measured in the spectral range of 135–190 nm. This range is dominated by lines in atomic nitrogen and lines formed by overlapping C2Σ+u(v') → X2Σ+g(v'') bands with Δv = const in the N+2 molecular ion which result from the spectator Auger decays of the N*2(1s−1π*(vr)) resonances. Ab initio calculations of the corresponding potential curves and transition probabilities showed that the observed irregular intensity dependence of the C2Σ+u(v') → X2Σ+g(v'')(Δv = const) fluorescence lines on the vibrational quantum number vr is due to transitions between vibrational levels during the reaction N2(v0 = 0)→ N*2(1s−1π*(vr)) Longrightarrow C2Σ+u(v') → X2Σ+g(v'')."}]}