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Shakeup excitation during optical tunnel ionization
I V Litvinyuk1, F Légaré, P W Dooley
1National Research Council of Canada, 100 Sussex Drive, Ottawa, Ontario, Canada K1A 0R6.
Physical Review Letters
|February 9, 2005
Summary
Strong infrared laser fields cause electron shakeup during tunnel ionization, exciting a second electron. This study develops a theory and experimental measurement, finding excellent agreement for the excited sigma(u) D(+)(2) state.
Area of Science:
- Atomic and Molecular Physics
- Quantum Mechanics
- Strong Field Physics
Background:
- Investigating electron dynamics in intense laser fields is crucial for understanding fundamental atomic and molecular processes.
- Tunnel ionization in strong fields leads to complex electron interactions, including shakeup phenomena.
- The behavior of two-electron systems under extreme electromagnetic conditions remains an active area of research.
Purpose of the Study:
- To theoretically and experimentally investigate the shakeup of a two-electron system in a strong infrared laser field.
- To develop a comprehensive analytical theory for shakeup in intense laser fields.
- To quantitatively measure and compare the shakeup process with theoretical predictions.
Main Methods:
- Development of a complete analytical theory for electron shakeup in intense laser fields.
- Experimental investigation using strong infrared laser fields.
- Utilizing the molecular clock, based on internuclear motion, for experimental shakeup measurement.
Main Results:
- Prediction of the formation of one excited sigma(u) D(+)(2) state per approximately 10(5) ionization events.
- Experimental observation of the predicted shakeup process.
- Quantitative agreement between the number of measured shakeup events and theoretical predictions.
Conclusions:
- The developed analytical theory accurately describes electron shakeup in intense laser fields.
- Experimental validation confirms the theory's predictions for the sigma(u) D(+)(2) state.
- The molecular clock is an effective tool for measuring shakeup phenomena in strong-field atomic physics.