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Analyzing the dependencies of refractive indices of nanocomposites on ZnS content (Figure 6), it can be seen that the dependence is linear and is fitted with effective media approximation, except for nanocomposites A13S, A14S, and A15S.
GLMMs were fit by the Laplace approximation.
Models were fit by maximum likelihood (Laplace Approximation) using a poisson error distribution.
The coefficients of an approximation equation considering ETT resistance were fitted separately to the measured pressure-flow curves for inspiration and expiration.
All variables are considered as fixed effects and the models were fit using Laplacian approximation [ 37].
Because AIC-based model selection requires maximum likelihood estimates [ 29], GLMM were fitted using the Gauss-Hermite approximation and the lme4 package for R software 2.12 [ 30], which gives the fitted model likelihood.
The model was fitted using a Laplacian approximation.
Both unfolding curves can be fitted using a two-state approximation with no folding intermediates detected.
The renormalized Maxwell-Garnett approximation was used to fit the experimental spectrum, using effective of optical parameters for the calculation.
The model was fit using the first-order conditional approximation to the likelihood in NONMEM.
(11)The goodness of fit of this approximation is examined in the Appendix.
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