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Floquet–Liouville supermatrix approach. II. Intensity-dependent generalized nonlinear optical susceptibilities

J. Chem. Phys. 86, 3225 (1987); doi:10.1063/1.451981

Issue Date: 15 March 1987

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Kwanghsi Wang and Shih-I Chu
Department of Chemistry, University of Kansas, Lawrence, Kansas 66045
We present a practical nonperturbative method for exact treatment of intensity-dependent generalized nonlinear optical susceptibilities chi(omega) in intense polychromatic fields, valid for arbitrary laser intensities, detunings, and relaxation. By means of the many-mode Floquet theory, the time-dependent Liouville equation can be transformed into an equivalent time-independent infinite-dimensional Floquet–Liouville supermatrix (FLSM) eigenvalue problem. It is then shown that the nonlinear optical susceptibilities chi(omega) can be completely determined simply from the supereigenvalues and eigenfunctions of the Floquet–Liouvillian L-hat F. In addition to this exact FLSM approach, we have also presented higher-order perturbative results, based on the extension of the Salwen's nearly degenerate perturbation theory, appropriate for somewhat weaker fields and near-resonant multiphoton processes, but beyond the conventional perturbative or rotating wave approximation (RWA). In the case of two-level systems, for example, the implementation of Salwen's method in the time-independent L-hat F allows the reduction of the infinite-dimensional FLSM into a 4×4 dimensional effective Hamiltonian, from which essential analytical formulas for intensity-dependent chi(omega) can be obtained. These methods are applied to a detailed study of intensity-dependent spectral line shapes (such as hole burning and extra resonance peaks at the line center, and the effects of saturation, detuning, and radiative and collisional damping, etc.) and subharmonic structures in nonlinear multiple wave mixings chi[(m+1)omega1momega2] for two-level systems in intense linearly polarized bichromatic fields. The Journal of Chemical Physics is copyrighted by The American Institute of Physics.
History: Received 15 August 1986; accepted 2 December 1986
Permalink: http://link.aip.org/link/?JCPSA6/86/3225/1
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KEYWORDS and PACS

Keywords
PACS
  • 42.65.-k
    Optics Nonlinear optics
  • 35.20.My
    Experimentally derived information on atoms and molecules; instrumentation and techniques Molecules Electric and magnetic moments (and derivatives), polarizability, and magnetic susceptibility
  • YEAR: 1987

PUBLICATION DATA

ISSN:
0021-9606 (print)   1089-7690 (online)
Publisher:
AIP is a member of CrossRef AIP

REFERENCES (20)

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  1. N. Bloembergen, Nonlinear Optics (Benjamin, New York, 1965).
  2. Y. R. Shen, The Principles of Nonlinear Optics (Wiley, New York, 1984).
  3. M. D. Levenson, Introduction to Nonlinear Laser Spectroscopy (Academic, New York, 1982).
  4. N. Tan-no, K. Okhawara, and H. Inaba, Phys. Rev. Lett. 46, 1282 (1981).
  5. L. Hillman, J. Krasinski, R. W. Boyd, and C. R. Stroud, Phys. Rev. Lett. 52, 1605 (1984).
  6. A. M. Bonch-Bruevich, S. G. Przhibelskii, and N. A. Chigir, Zh. Eksp. Teor. Phys. 80, 565 (1981)
  7. [Sov. Phys. JETP 53, 285 (1981)];
  8. A. M. Bonch-Bruevich, T. A. Vartanyan, and N. A. Chigir, ibid. 77, 1899 (1979)
  9. [50, 901 (1979)].
  10. R. K. Raj, Q. F. Gao, D. Bloch, and M. Ducloy, Opt. Commun. 51, 117 (1984).
  11. G. I. Toptygina and E. E. Fradkin, Zh. Eskp. Teor. Phys. 82, 429 (1982)
  12. [Sov. Phys. JETP 55, 246 (1982)].
  13. G. S. Agarwal and N. Nayak, Phys. Rev. A 33, 391 (1986);
  14. M. S. Kumar and G. S. Agarwal, ibid. 33, 1817 (1986).
  15. B. Dick and R. M. Hochstrasser, Chem. Phys. 75, 133 (1983).
  16. T.-S. Ho, K. Wang, and S.-I. Chu, Phys. Rev. A 33, 1798 (1986).
  17. U. Fano, Phys. Rev. 131, 259 (1963).
  18. (a) T.-S. Ho, S.-I. Chu, and J. V. Tietz, Chem. Phys. Lett. 99, 422 (1983);
  19. (b) S.-I. Chu and T.-S. Ho, Isr. J. Chem. 24, 237 (1984);
  20. (c) T.-S. Ho and S.-I. Chu, J. Phys. B 17, 2101 (1984);
  21. (d) Phys. Rev. A 31, 659 (1985);
  22. (e) 32, 377 (1985).
  23. For a recent review on Floquet approaches, see, S.-I. Chu, Adv. At. Mol. Phys. 21, 197 (1985), and references therein.
  24. H. Salwen, Phys. Rev. 99, 1274 (1955).
  25. K. Wang, T.-S. Ho, and S.-I. Chu, J. Phys. B 18, 4539 (1985).
  26. L. W. Hillman, R. W. Boyd, J. Krasinski, and C. R. Stroud, Jr., Opt. Commun. 45, 416 (1983).
  27. R. W. Boyd and S. Mukamel, Phys. Rev. A 29, 1973 (1984).
  28. (a) R. E. Walkup, A. Spielfieldel, and D. E. Pritchard, Phys. Rev. Lett. 45, 986 (1980);
  29. (b) J. F. Kielkopf and N. F. Allard, J. Phys. B 13, 709 (1980).
  30. G. S. Agarwal and N. Nayak, J. Opt. Soc. Am. B 1, 164 (1984).

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