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Volumn 13, Issue 3, 1996, Pages 496-513

Femtosecond continuum interferometer for transient phase and transmission spectroscopy

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EID: 0030558989     PISSN: 07403224     EISSN: None     Source Type: Journal    
DOI: 10.1364/JOSAB.13.000496     Document Type: Article
Times cited : (37)

References (44)
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    • Rodenberger, D.C.1    Grossman, C.H.2    Garito, A.F.3
  • 19
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    • Department of Physics, University of Pennsylvania, Philadelphia, Pa., 19104 personal communication
    • D. C. Rodenberger, C. H. Grossman, and A. F. Garito, Opt. Lett 15, 498 (1990); and D. C. Rodenberger, Department of Physics, University of Pennsylvania, Philadelphia, Pa., 19104 (personal communication, 1991).
    • (1991)
    • Rodenberger, D.C.1
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    • Knox, W.H.1
  • 23
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    • note
    • The position of zero delay is determined from the t-v curve in Fig. 7 below.
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    • D. McMorrow, W. T. Lotshaw, and G. A. Kenney-Wallace, IEEE J. Quantum Electron. 24, 443 (1988); C. Kalpouzos, D. McMorrow, W. T. Lotshaw, and G. A. Kenney-Wallace, Chem. Phys. Lett. 150, 138 (1988); Commun. Chem. Phys. Lett. 155, 240 (1989).
    • (1989) Commun. Chem. Phys. Lett. , vol.155 , pp. 240
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    • R. R. Alfano and P. P. Ho, IEEE J. Quantum Electron. 24, 351 (1988); R. R. Alfano, The Supercontinuum Laser Source (Springer-Verlag, New York, 1989).
    • (1988) IEEE J. Quantum Electron. , vol.24 , pp. 351
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    • Springer-Verlag, New York
    • R. R. Alfano and P. P. Ho, IEEE J. Quantum Electron. 24, 351 (1988); R. R. Alfano, The Supercontinuum Laser Source (Springer-Verlag, New York, 1989).
    • (1989) The Supercontinuum Laser Source
    • Alfano, R.R.1
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    • S. L. Shapiro, ed. Springer-Verlag, New York
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    • (1977) Ultrashort Light Pulses , pp. 83
    • Ippen, E.P.1    Shank, C.V.2
  • 39
    • 3843088083 scopus 로고    scopus 로고
    • note
    • eff in Eq. (30), of the chirped continuum is correspondingly broader than the spectral width of the fundamental pulse in this case. Of course, if the continuum is filtered to have exactly the same spectral width as the fundamental, the filtered pulse has a longer duration that the fundamental because it is not FT limited.
  • 44
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    • note
    • In this paper the propagation effect is ignored. When a δ-function probe pulse is incident upon a sample, the sample thickness must always be taken into account. Then the unperturbed probe pulse without excitation suffers deformation because of the linear absorption or dispersion effects during propagation and cannot be regarded as a δ function in the sample. As a result, the pump-induced change causes modulation effects and does not strictly satisfy the causality condition. Therefore the discussion here is valid when the propagation effect is not significant.


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