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Transition from SAMO to Rydberg State Ionization in C(60) in Femtosecond Laser Fields

[Image: see text] The transition between two distinct ionization mechanisms in femtosecond laser fields at 785 nm is observed for C(60) molecules. The transition occurs in the investigated intensity range from 3 to 20 TW/cm(2) and is visualized in electron kinetic energy spectra below the one-photon...

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Detalles Bibliográficos
Autores principales: Li, H., Mignolet, B., Wang, Z., Betsch, K. J., Carnes, K. D., Ben-Itzhak, I., Cocke, C. L., Remacle, F., Kling, M. F.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2016
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5190148/
https://www.ncbi.nlm.nih.gov/pubmed/27934203
http://dx.doi.org/10.1021/acs.jpclett.6b02139
Descripción
Sumario:[Image: see text] The transition between two distinct ionization mechanisms in femtosecond laser fields at 785 nm is observed for C(60) molecules. The transition occurs in the investigated intensity range from 3 to 20 TW/cm(2) and is visualized in electron kinetic energy spectra below the one-photon energy (1.5 eV) obtained via velocity map imaging. Assignment of several observed broad spectral peaks to ionization from superatom molecular orbitals (SAMOs) and Rydberg states is based on time-dependent density functional theory simulations. We find that ionization from SAMOs dominates the spectra for intensities below 5 TW/cm(2). As the intensity increases, Rydberg state ionization exceeds the prominence of SAMOs. Using short laser pulses (20 fs) allowed uncovering of distinct six-lobe photoelectron angular distributions with kinetic energies just above the threshold (below 0.2 eV), which we interpret as over-the-barrier ionization of shallow f-Rydberg states in C(60).