Abstract
The study of the interaction of intense laser fields with atoms and molecules has attracted considerable attention in recent years. In particular, the availability of increasingly intense lasers has made possible the observation of a wide variety of multiphoton processes, including multiphoton ionization, laser-assisted electron–atom collisions and harmonic generation. Also, in the case of molecules, the loss of spherical symmetry and the degrees of freedom associated with the nuclear motion give rise to additional computational difficulties and new effects including multiphoton dissociation. Many reviews of these processes have been written and we mention here comprehensive overviews by Gavrila [365], Burnett et al. [194], Mason [639], Protopapas et al. [759] and Joachain et al. [504] where the emphasis is on atomic multiphoton processes, and by Bandrauk et al. [50, 51], Giusti-Suzor et al. [378] and Posthumus [751], where the emphasis is on molecular multiphoton processes.
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- 1.
Explicit expressions for the potential matrices \(\textbf{ V}^{E\gamma}\), V Dγ and \(\textbf{V}^{P\gamma}\) in (9.41) are derived in Appendix D.2.
- 2.
See Sect. 9.2.3 for a further discussion of LICS states.
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Burke, P.G. (2011). Multiphoton Processes: Floquet Theory. In: R-Matrix Theory of Atomic Collisions. Springer Series on Atomic, Optical, and Plasma Physics, vol 61. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-15931-2_9
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