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Line Raman, Rayleigh, and laser-induced predissociation fluorescence technique for combustion with a tunable KrF excimer laser
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One-dimensional, time-resolved Raman measurements in a sooting flame made with 355-nm excitation
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J. O. Gilmore, S. Sharma, D. Fletcher, and D. Bershader, "Single-pulse spontaneous Raman scattering measurements in an expanding nitrogen/oxygen admixture," paper AIAA-95-2125, presented at the 30th AIAA Thermophysics Conference, San Diego, Calif., 19-22 June, 1995 (American Institute for Aeronautics and Astronautics, Reston, Va., 1995).
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18
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84893992318
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note
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Unless explicitly stated otherwise, the integration limits will be from -∞ to + ∞ for (reciprocal) space coordinates and from 0 to +∞ for wavelengths and frequencies.
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19
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84894012546
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note
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out).
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20
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84894006473
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note
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The line at λ = 579.40 nm is an unresolved doublet. In fact, the exact wavelengths used do not matter for the processing of OMA graphs.
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24
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84893992245
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note
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As input signal S(x) of the FT is purely real, the Fourier-transformed data S̄̃(k) are even under complex conjugation; i.e., S̄̃(-k) = S̄̃*(k). Therefore, only the positive k components need to be plotted to represent all power information.
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29
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0003531188
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30
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84894000541
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note
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This is a general property of Fourier transformation. For visual clarity, the reconstructions presented in this paper (Figs. 4 and 6) have been recentered in the image frames.
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32
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84894003357
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See, e.g., Ref. 1, Sec. 3.6
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See, e.g., Ref. 1, Sec. 3.6.
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33
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0003474751
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Cambridge U. Press, Cambridge, Mass.
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W. H. Press, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numerical Recipes in C - The Art of Scientific Computation, 2nd ed. (Cambridge U. Press, Cambridge, Mass., 1992).
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Flannery, B.P.4
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34
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84893990953
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note
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2 = S × S*), and the norm of the signal ∥S∥ is the integral over S.
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