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The second-harmonic intensity from alternate-layer Langmuir−Blodgett films of a coumarin dye, 4-[2-(7-diethylamino-2-oxo-2 H -benzopyran-3-yl)ethenyl]-1-octadecylquinolinium bromide, and an inert spacer, 1-octadecyl-4-methylquinolinium bromide, increases quadratically with the number of active layers. The optimum effective second-order susceptibility, albeit resonantly enhanced, is the highest to date for a thick alternate-layer film with χ eff (2) = 190 ± 30 pm V - 1 at 1.064 μm. The thickness and the real and imaginary components of the dielectric permittivity from the surface plasmon resonance at 532 nm are l = 4.6 ± 0.4 nm bilayer - 1, ε r = 2.4 ± 0.2 and ε i = 0.8 ± 0.2.
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Ashwell et al. (1998) studied this question.
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