1992
DOI: 10.1017/s0263034600004304
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Tunnel ionization of K and Xe atoms by an intense CO2 laser

Abstract: The energy spectra of electrons emitted radially from a CO 2 laser focus originating from the ionization of K and Xe atoms of tenuous gas pressure are measured. We simultaneously measured the cases in which medium laser intensities and high laser intensities are applied, fitting the ADK tunneling theory.

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Cited by 6 publications
(6 citation statements)
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“…This theory (i.e. quasistatic tunnelling) has previously been successfully used (Xiong and Chin 1991, Corkum eta/ 1989, Augst eta1 1991 to describe the tunnelling behaviour in atoms, however, in this paper, its scope of validity has been extended into the realm of non-resonant simple molecules (i.e. diatomic and triatomic).…”
Section: Discussionmentioning
confidence: 99%
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“…This theory (i.e. quasistatic tunnelling) has previously been successfully used (Xiong and Chin 1991, Corkum eta/ 1989, Augst eta1 1991 to describe the tunnelling behaviour in atoms, however, in this paper, its scope of validity has been extended into the realm of non-resonant simple molecules (i.e. diatomic and triatomic).…”
Section: Discussionmentioning
confidence: 99%
“…That is to say that no intermediate levels enter into the picture between the initial state of the atomic system and the final state in the continuum in this quasi-static tunnel ionization model. The scope of the concordance between this model and experiment has been tested through electron spectra (Corkum etaf 1989, Xiong and Chin 1991. ion yields for both singly Chin 1991, 1992) and multiply charged ions (Augst et a1 1991, Auguste et a1 1992) and using a variety of different laser characteristics (e.g.…”
Section: Introductionmentioning
confidence: 99%
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“…There are several analytical tunneling models [2,3]. One of the most used, the Amosov-Delone-Krainov (ADK), gives good agreement with the time dependent Schrodinger equa tion [4,5] and excellent agreement with experimental results [6]. This model for a linearly polarized laser field and the non zero initial momentum, p, of ejected photoelectrons describes the transition ionization rate as an exponential dependence on the field strength, F, the ionization potential of state, E i , the effective principle quantum number, n * [7]:…”
Section: Introductionmentioning
confidence: 99%