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Volumn 62, Issue 3, 2000, Pages 033820-033821

Phase-resolved time-domain nonlinear optical signals

Author keywords

[No Author keywords available]

Indexed keywords

COMPUTER SIMULATION; ELECTRIC FIELDS; ELECTRON ENERGY LEVELS; GREEN'S FUNCTION; LASER PULSES; LIGHT MODULATION; LIGHT POLARIZATION; MOLECULAR DYNAMICS; NUMERICAL ANALYSIS; PERTURBATION TECHNIQUES; RAMAN SCATTERING; ULTRAFAST PHENOMENA;

EID: 0000696321     PISSN: 10502947     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article
Times cited : (35)

References (98)
  • 40
    • 21144465387 scopus 로고
    • Some results in this paper differ superficially from those given here, because Lee and Albrecht defined the phase of the nonlinear polarization as the signed sum of the excitation pulse phases, and incorporated the phase of the susceptibility into the phase shift between the polarization and emitted field
    • D. Lee and A. C. Albrecht, Adv. Chem. Phys. 83, 43 (1993). Some results in this paper differ superficially from those given here, because Lee and Albrecht defined the phase of the nonlinear polarization as the signed sum of the excitation pulse phases, and incorporated the phase of the susceptibility into the phase shift between the polarization and emitted field.
    • (1993) Adv. Chem. Phys. , vol.83 , pp. 43
    • Lee, D.1    Albrecht, A.C.2
  • 48
    • 0000984401 scopus 로고    scopus 로고
    • This experiment was based on signal intensity modulation with delay between a collinear pulse pair where the wave vector of the pulse pair appears only once in the signal wave vector. In all the other experiments discussed here, the wave vector of each pulse appears separately in the signal wave vector
    • J. A. McGuire, W. Beck, X. Wei, and Y. R. Shen, Opt. Lett. 24, 1877 (1999). This experiment was based on signal intensity modulation with delay between a collinear pulse pair where the wave vector of the pulse pair appears only once in the signal wave vector. In all the other experiments discussed here, the wave vector of each pulse appears separately in the signal wave vector.
    • (1999) Opt. Lett. , vol.24 , pp. 1877
    • McGuire, J.A.1    Beck, W.2    Wei, X.3    Shen, Y.R.4
  • 58
    • 0343321983 scopus 로고    scopus 로고
    • note
    • 6 in the limit of vanishing damping.
  • 65
    • 0003434416 scopus 로고
    • University Science Books, Mill Valley, CA
    • A. E. Siegman, Lasers (University Science Books, Mill Valley, CA, 1986).
    • (1986) Lasers
    • Siegman, A.E.1
  • 84
    • 0342452625 scopus 로고    scopus 로고
    • note
    • n(x) yields ∫ δo(x)θ(x)dx = 1/2. When improperly time-ordered diagrams are included, this evaluation of the δ-function integrals at discontinuities naturally leads to analytic results that agree with numerical integration over sufficiently short symmetric pulses. At T=0, these δ-function results differ from those given previously by us [36] and others. [41,60] For consistency, a limiting series of integrals could also be used to define the response function in terms of the polarization at discontinuities.
  • 87
    • 0343757957 scopus 로고    scopus 로고
    • Ph.D. thesis, University of Colorado, Boulder, CO
    • S. M. Gallagher Faeder, Ph.D. thesis, University of Colorado, Boulder, CO, 1999.
    • (1999)
    • Gallagher Faeder, S.M.1
  • 90
    • 0342452624 scopus 로고    scopus 로고
    • note
    • p, but this prediction could be experimentally tested with transform-limited broadband excitation of a narrow resonance.
  • 93
    • 0342887066 scopus 로고    scopus 로고
    • note
    • 0) and the transition dipole product. This is known as phase cycling in NMR [70].


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.