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Dyke JM. Photoionization studies of reactive intermediates using synchrotron radiation. Phys Chem Chem Phys 2019; 21:9106-9136. [DOI: 10.1039/c9cp00623k] [Citation(s) in RCA: 16] [Impact Index Per Article: 3.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/21/2022]
Abstract
Photoionization with synchrotron radiation enables sensitive and selective monitoring of reactive intermediates in environments such as flames and plasmas.
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Schnorr K, Senftleben A, Kurka M, Rudenko A, Schmid G, Pfeifer T, Meyer K, Kübel M, Kling MF, Jiang YH, Treusch R, Düsterer S, Siemer B, Wöstmann M, Zacharias H, Mitzner R, Zouros TJM, Ullrich J, Schröter CD, Moshammer R. Electron rearrangement dynamics in dissociating I(2)^(n+) molecules accessed by extreme ultraviolet pump-probe experiments. PHYSICAL REVIEW LETTERS 2014; 113:073001. [PMID: 25170702 DOI: 10.1103/physrevlett.113.073001] [Citation(s) in RCA: 17] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/07/2014] [Indexed: 05/11/2023]
Abstract
The charge rearrangement in dissociating I_{2}^{n+} molecules is measured as a function of the internuclear distance R using extreme ultraviolet pulses delivered by the free-electron laser in Hamburg. Within an extreme ultraviolet pump-probe scheme, the first pulse initiates dissociation by multiply ionizing I_{2}, and the delayed probe pulse further ionizes one of the two fragments at a given time, thus triggering charge rearrangement at a well-defined R. The electron transfer between the fragments is monitored by analyzing the delay-dependent ion kinetic energies and charge states. The experimental results are in very good agreement with predictions of the classical over-the-barrier model demonstrating its validity in a thus far unexplored quasimolecular regime relevant for free-electron laser, plasma, and chemistry applications.
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Affiliation(s)
- K Schnorr
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - A Senftleben
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - M Kurka
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - A Rudenko
- J.R. Macdonald Laboratory, Kansas State University, Manhattan, Kansas 66506, USA
| | - G Schmid
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - T Pfeifer
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - K Meyer
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - M Kübel
- Max-Planck-Institut für Quantenoptik, 85748 Garching, Germany
| | - M F Kling
- J.R. Macdonald Laboratory, Kansas State University, Manhattan, Kansas 66506, USA and Max-Planck-Institut für Quantenoptik, 85748 Garching, Germany
| | - Y H Jiang
- Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai 201210, China
| | - R Treusch
- Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany
| | - S Düsterer
- Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany
| | - B Siemer
- Westfälische Wilhelms-Universität, 48419 Münster, Germany
| | - M Wöstmann
- Westfälische Wilhelms-Universität, 48419 Münster, Germany
| | - H Zacharias
- Westfälische Wilhelms-Universität, 48419 Münster, Germany
| | - R Mitzner
- Helmholtz-Zentrum Berlin, 12489 Berlin, Germany
| | - T J M Zouros
- Department of Physics, University of Crete, Post Office Box 2208, 71003 Heraklion, Crete, Greece
| | - J Ullrich
- Physikalisch-Technische Bundesanstalt, 38116 Braunschweig, Germany
| | - C D Schröter
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
| | - R Moshammer
- Max-Planck-Institut für Kernphysik, 69117 Heidelberg, Germany
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