Statistical fragmentation of doubly charged anthracene induced by fluorine-beam impact at 3 keV

The fragmentation scheme of the doubly charged anthracene molecule (C 14 H 10 2+) has been studied via monocharged fluorine impact at 3 keV using the CIDEC method (collision-induced dissociation under energy control). Doubly or singly charged fragments resulting from the loss of neutrals (H, C 2 H 2...

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Veröffentlicht in:Physical review. A 2012-05, Vol.85 (5), Article 052715
Hauptverfasser: Martin, S., Chen, L., Brédy, R., Montagne, G., Ortega, C., Schlathölter, T., Reitsma, G., Bernard, J.
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Sprache:eng
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Zusammenfassung:The fragmentation scheme of the doubly charged anthracene molecule (C 14 H 10 2+) has been studied via monocharged fluorine impact at 3 keV using the CIDEC method (collision-induced dissociation under energy control). Doubly or singly charged fragments resulting from the loss of neutrals (H, C 2 H 2) or C x H y + (x = 1-5; y = 1-5) have been measured versus the excitation energy of the parent molecule C 14 H 10 2+. The branching ratio of the C x H y + emission process was found to be 16%. For the major neutral evaporation channels via nH or nC 2 H 2 (n = 1, 2) emission, the measured population distributions have been fitted using a Rice-Ramsperger-Kassel (RRK) statistical dissociation and cascade model. The simulated rate-energy dependences of the two primary competing pathways, i.e., the loss of H or C 2 H 2 from C 14 H 10 2+ , present a crossing point at 13 eV. This feature is characteristic of two different fragmentation mechanisms: a direct cleavage for the loss of H for energy above the crossing point and a rearrangement process for the loss of C 2 H 2 bellow the crossing point.
ISSN:1050-2947
2469-9926
1094-1622
2469-9934
DOI:10.1103/PhysRevA.85.052715