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Figure 4 displays the binding energy as a function of the height of dot, L d, for different impurity positions.
In Figure 6, the variation of the binding energy as a function of L d and in the presence of magnetic field is shown.
The ground-exciton binding energy as a function of x Al 1 (Figure1b) shows initially a decreasing behavior until the left-hand-barrier Al composition is approximately 0.18.
Figure1 shows the dependence of the ground (n e = 1 and n h = 1) exciton binding energy as a result of the variation of the left-hand-barrier Al composition x Al 1.
Figure2 contains our results for the heavy-hole exciton binding energy as a function of the QW width, without the application of any dc electric field and taking several values of theα0 as a parameter.
If an intense laser field is applied taking the QW geometry as a varying parameter, the results obtained for the heavy-hole exciton binding energy as a function ofα0 are those shown in the Figure3.
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By quantifying the potential-dependent behavior of all products, we provide insights into kinetics and mechanisms at play, in particular involving the production of hydrocarbons and alcohols on catalysts with weak CO binding energy as well as the formation of a C-C bond required to produce ethanol.
In second part of this investigation, a set of new allosteric MEK1/2 inhibitors were designed significantly improving the binding energy as well as the ADMET properties, suggesting more specific and stable ligand-receptor complexes.
(6)–(8), and (5) the binding energy, as well as in [26], is found as the difference E b (R,B) = E 01 − E i (R,B).
The negative and lower value of binding energy as well as more numbers of hydrogen bonds showed favored binding between ligand and target.
This docking study of the 40S ribosomal S9 protein showed that out of 10 docked conformations, the 3rd conformation was the best because it has comparatively lower binding energy as well as hydrogen bonding.
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