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The geometries of the chromophores were optimized using a semiempirical AM1 method as implemented in the MOPAC 3.1 package. Dewar, M. J. S.; Zoebisch, E. G.; Healy, E. F.; Stewart, J. J. P. J. Am. Chem. Soc. 1985, 107, 3902.
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33746330593
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note
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-30 was used for conversion. Comparison of β for all chromophores at a single excitation wavelength, say 1.9 μm, is not useful because of various resonance effects, resulting from the wide range of spectral windows between chromophores.
-
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59
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33746324986
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note
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We thank a reviewer for clarifying that the intermolecular electronic interactions and the poling field on individual molecules cannot be treated independently when we generate an acentric order by applying an external poling field.
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note
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As a reviewer suggested, luminescence is a common issue with HRS measurements, But interference from the luminescence of TCP chromophores is not a complication in these measurements. Because we use a spectrograph to disperse the radiation coming from the sample, we can discern the multiphoton-excited fluorescence background from the HRS signal through analysis of the line width. In these experiments, the HRS intensity was sufficiently intense relative to the luminescence background that it could be readily identified and measured.
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