Abstract
The excitation of atoms by intense laser pulses can be divided into two broad regimes: the first regime involves relatively weak optical laser fields of long duration, and the second involves strong fields of short duration. In the first case, the intensity is presumed to be high enough for multiphoton transitions to occur. The resulting spectroscopy is not limited by the single-photon selection rules for radiative transitions. However, the intensity is still low enough for a theoretical description based on perturbations of field-free atomic states to be valid, and the time dependence of the field amplitude does not play an essential role. In the second case, the field intensities are too large to be treated by perturbation theory, and the time dependence of the pulse must be taken into account. A discussion on the generation of sub-femtosecond pulses is included.
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Abbreviations
- ATI:
-
above threshold ionization
- HG:
-
harmonic generation
- PDM:
-
phase diffusion model
- REMPI:
-
resonance-enhanced multiphoton ionization
- SS:
-
strong-short
- TDSE:
-
time dependent Schrödinger equation
- UV:
-
ultraviolet
- WL:
-
weak-long
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Acknowledgements
This work was supported in part by the U.S. DOE under contract number W-7405-ENG-48.
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Kulander, K., Lewenstein, M. (2006). Multiphoton and Strong-Field Processes. In: Drake, G. (eds) Springer Handbook of Atomic, Molecular, and Optical Physics. Springer Handbooks. Springer, New York, NY. https://doi.org/10.1007/978-0-387-26308-3_74
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