Control of H2 dissociative ionization in the nonlinear regime using vacuum ultraviolet free-electron laser pulses

The role of the nuclear degrees of freedom in nonlinear two-photon single ionization of H2 molecules interacting with short and intense vacuum ultraviolet pulses is investigated, both experimentally and theoretically, by selecting single resonant vibronic intermediate neutral states. This high selec...

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Detalles Bibliográficos
Autores: Holzmeier, F., Bello Romero, Roger Yulier, Hervé, M., Achner, A., Baumann, T. M., Meyer, M., Finetti, P., Di Fraia, M., Gauthier, D., Roussel, E., Plekan, O., Richter, R., Prince, K. C., Callegari, C., Bachau, H., Palacios Cañas, Alicia, Martín García, Fernando, Dowek, D.
Tipo de recurso: artículo
Fecha de publicación:2018
País:España
Institución:Universidad Autónoma de Madrid
Repositorio:Biblos-e Archivo. Repositorio Institucional de la UAM
Idioma:inglés
OAI Identifier:oai:repositorio.uam.es:10486/685783
Acceso en línea:http://hdl.handle.net/10486/685783
https://dx.doi.org/10.1103/PhysRevLett.121.103002
Access Level:acceso abierto
Palabra clave:Nonlinear
Ionization of H2
Vacuum
Ultraviolet pulse
Electron laser
Dissociative ionization
Química
Descripción
Sumario:The role of the nuclear degrees of freedom in nonlinear two-photon single ionization of H2 molecules interacting with short and intense vacuum ultraviolet pulses is investigated, both experimentally and theoretically, by selecting single resonant vibronic intermediate neutral states. This high selectivity relies on the narrow bandwidth and tunability of the pulses generated at the FERMI free-electron laser. A sustained enhancement of dissociative ionization, which even exceeds nondissociative ionization, is observed and controlled as one selects progressively higher vibronic states. With the help of ab initio calculations for increasing pulse durations, the photoelectron and ion energy spectra obtained with velocity map imaging allow us to identify new photoionization pathways. With pulses of the order of 100 fs, the experiment probes a timescale that lies between that of ultrafast dynamical processes and that of steady state excitations