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The solid lines in both panels represent fittings to the single-level tunnelling transport model in equation (1) with the parameters given in Table 1.
(b) Corresponding response of the junction as calculated from the single-level tunnelling transport model in equation (1) using the parameters given in Table 1.
In this paper we propose to tackle all these models using generalized disjunctive programming to capture the numerical characteristics of each model (in equation form, modular, noisy, etc).
Therefore, for the remainder of this study we used the gravity model in Equation (2).
The results obtained by estimating the model in equation 5 are reported in Table 8.
The measurement model in Equation 1 and the random signal model are adopted.
Some consideration on the linear model in Equation 6 should now be done.
The extended reflection model in Equation 4 is the same fashion mathematically as the standard model in Equation 3 for dielectric, although the two reflection models are physically different.
The results of estimating the difference in-differences modifference in-differenceseported in Table 615.
The Adj. R 2 = .053 indicates the total variance in emergent strategy explained by the regression model in Equation 3.
The compounding procedure follows by taking the E W class (3) as the baseline model in Equation (2).
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