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The extinction coefficient presented here is a weighted average of two tautomers; see the following sections
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This assumption was also made in ref 18 for estimation of the first and second hyperpolarizabilities and |Δμ01| value for NSPc. A good agreement (Table 1) between the |Δμ01| value found with this method in ref 18 and that obtained from eqs 9 and 10, which do not include the angle between μ0 and Δμ10, proves the assumption. Furthermore, quantum-mechanical calculations of the similar molecules in ref 15 show that the absolute angle between μ0 and & (Δμ20) is not larger than 27°, which can result in an additional error of μ0 not larger than 10, i.e, less than the total error claimed in Table 1. The angle a between Δμf0 and μf0 was calculated15 to be either 2° or 64° for the first two transitions. The last value, if substituted in eq 17, will produce an error (overestimate of σ2) of 38, whi
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2, claimed in Table 2.
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