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Volumn 82, Issue 1, 2010, Pages

Simulation of the above-threshold-ionization experiment using the molecular strong-field approximation: The choice of gauge

Author keywords

[No Author keywords available]

Indexed keywords

EXPERIMENTAL DATA; INITIAL STATE; IONIZATION YIELD; LASER FIELDS; LOW-ENERGY SPECTRA; STRONG-FIELD APPROXIMATIONS;

EID: 77954857370     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.82.015401     Document Type: Article
Times cited : (29)

References (21)
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    • The term "modified" is introduced to distinguish our molecular strong-field approximation theory from the standard MSFAs [4,5]. Our modified MSFA includes an additional term and enables laser-field dressing of the initial states. In [8], we have introduced four versions of the modified MSFA, while in the present work we show that the so-called dML version is superior to the standard MSFAs and to the other three versions of the modified MSFA. The term "improved" has the same meaning as for the improved SFA for atoms; that is, inclusion of an additional interaction of the ionized electron with the parent (atomic or molecular) ion via its rescattering off this core.
    • The term "modified" is introduced to distinguish our molecular strong-field approximation theory from the standard MSFAs [4,5]. Our modified MSFA includes an additional term and enables laser-field dressing of the initial states. In [8], we have introduced four versions of the modified MSFA, while in the present work we show that the so-called dML version is superior to the standard MSFAs and to the other three versions of the modified MSFA. The term "improved" has the same meaning as for the improved SFA for atoms; that is, inclusion of an additional interaction of the ionized electron with the parent (atomic or molecular) ion via its rescattering off this core.
  • 10
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    • The absence of this suppression was an argument that the velocity-gauge MSFA is superior to the length-gauge MSFA. We show here that this argument cannot be used for our dressed modified length-gauge MSFA, since it leads to the correct suppression factor, Eq. (1).
    • The absence of this suppression was an argument that the velocity-gauge MSFA is superior to the length-gauge MSFA. We show here that this argument cannot be used for our dressed modified length-gauge MSFA, since it leads to the correct suppression factor, Eq. (1).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.