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Volumn 56, Issue 5, 1997, Pages 3961-3973

High-frequency Floquet-theory content of wave-packet dynamics

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EID: 4243804939     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.56.3961     Document Type: Article
Times cited : (27)

References (49)
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    • See, for example, the volume Atoms in Intense Laser Fields, edited by M. Gavrila (Academic, New York, 1992).
    • See, for example, the volume Atoms in Intense Laser Fields, edited by M. Gavrila (Academic, New York, 1992).
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    • PRLTAO
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    • PRLTAO (b) for ionization see M. Gavrila, in Fundamentals of Laser Interactions, edited by F. Ehlotzky, Lecture Notes in Physics Vol. 229 (Springer, Berlin, 1985), p. 3.
    • (a) For free-free transitions see M. Gavrila and J. Z. Kaminski, Phys. Rev. Lett. 52, 614 (1984); PRLTAO(b) for ionization see M. Gavrila, in Fundamentals of Laser Interactions, edited by F. Ehlotzky, Lecture Notes in Physics Vol. 229 (Springer, Berlin, 1985), p. 3.
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    • PLRAAN
    • The relationship of the HFFT with the standard version of Floquet theory was studied recently by M. Marinescu and M. Gavrila, Phys. Rev. A 53, 2513 (1996).PLRAAN
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    • PRLTAO see also J. H. Eberly, R. Grobe, C. K. Law, and Q. Su, in Atoms in Intense Laser Fields (Ref.
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    • PRLTAO see also Atoms in Intense Laser Fields (Ref.
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    • SPHDA9 see also P. Kuchment, Floquet Theory for Partial Differential Equations (Birkhäuser, Basel, 1993), Sec. 5.5.
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    • A rigorous analysis of the quasienergy spectrum for one-electron atoms was given by K. Yajima, Commun. Math. Phys. 87, 331 (1982); CMPHAY
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    • S. Graffi and K. Yajima, 89, 277 (1983), for the case of linear polarization;
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    • JPHAC5
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    • PLRAAN
    • Population analyses have also been made in WPD in terms of field-free states; e.g., see M. Dörr, O. Latinne, and C. J. Joachain, Phys. Rev. A 52, 4289 (1995). Obviously, these populations have physical meaning only at the end of the pulse.PLRAAN
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    • NUCIAD see H. A. Kramers, Collected Scientific Papers (North-Holland, Amsterdam, 1956), p. 866;
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    • Pauli, W.1    Fierz, M.2
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    • The structure equation (6) was written down by W. C. Henneberger 19, but it was J. I. Gersten and M. H. Mittleman, J. Phys. B 9, 2561 (1976), who recognized its high-frequency character.JPAMA4
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    • Wiley, New York
    • For continuum normalization in the energy scale, see E. Merzbacher, Quantum Mechanics (Wiley, New York, 1970), Chap. 6, Sec. 3.
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    • NUPABL See also Berggren’s contribution to the volume Resonances, edited by E. Brändas and N. Elander, Lecture Notes in Physics Vol. 325 (Springer, Berlin, 1988), p. 106, and other articles in the same volume for the background of the problem.
    • The proof was given by T. Berggren, Nucl. Phys. A 109, 265 (1968), with the α-decay problem of nuclear physics in view. NUPABLSee also Berggren’s contribution to the volume Resonances, edited by E. Brändas and N. Elander, Lecture Notes in Physics Vol. 325 (Springer, Berlin, 1988), p. 106, and other articles in the same volume for the background of the problem.
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    • For example, see A. Messiah, Quantum Mechanics (North-Holland, Amsterdam, 1962), Chap. XVI, Eqs. 5, 6, 10, 13, 14, 26, and 27. Note that our (Formula presented) is denoted there by (Formula presented).
    • For example, see A. Messiah, Quantum Mechanics (North-Holland, Amsterdam, 1962), Chap. XVI, Eqs. 5, 6, 10, 13, 14, 26, and 27. Note that our (Formula presented) is denoted there by (Formula presented).


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