Time-resolved scattering media

J. C. Hebden, R.A. Kruger, K.S. Wong Time-resolved unaging through a highly scattering medium. Appl. Opt. 30, 788 (1991)... [Pg.572]

Fig. 3.5 Schematic (t (o) for an insulator-metal composite made up of volume fractions /of a Drude metal and 1 - / of an insulator, as calculated in the effective medium theory. The heavy line at w = 0 represents the Drude peak. The integrated stength of the delta function is proportional to the height of the delta function. The scattering time is chosen to be very long so that the width of the Drude peak is too narrow to be resolved in the plot, emphasizing the behavior of the localized modes. (From Ref. 88.)...

$Fig. 3.5 Schematic (t (o) for an insulator-metal composite made up of volume fractions /of a Drude metal and 1 - / of an insulator, as calculated in the effective medium theory. The heavy line at w = 0 represents the Drude peak. The integrated stength of the delta function is proportional to the height of the delta function. The scattering time is chosen to be very long so that the width of the Drude peak is too narrow to be resolved in the plot, emphasizing the behavior of the localized modes. (From Ref. 88.)...$

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