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Energy decomposition analysis from the FMO calculation reveals that the majority of the energy comes from the charge transfer contribution of charged atoms.
To evaluate the contribution of charged residues responsible for dimerization properties of BdbZIPs, the frequency of attractive and repulsive g↔e pairs in each heptad of BdbZIP leucine zippers was computed and the corresponding histogram was demonstrated.
To analyze the contribution of charged residues to the dimerization properties of the legume bZIP proteins, we calculated the frequency of attractive and repulsive g↔ eʹ pairs in each heptad of the bZIP Leu zippers; the corresponding histograms are shown in Fig. 4c.
To analyse the contribution of charged residues at the e and g positions in governing dimerization properties of ZmbZIP proteins, we calculate the presence of attractive and repulsive g↔e′ pairs in each heptad of maize leucine zippers (Supplementary Fig. S7), and the histogram of their frequency is presented in Fig. 2F.
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It is argued that the contributions of charged particles and AlN dimers are the origin of the discrepancy.
Moreover, the contribution from kaons is large (∼80%) as compared to the contribution from decay of charged pions (∼20%).
However, the contribution of charge transfer on the enthaplic binding term is dependent on the wave function used.
Single cells fabricated with electroless AAL show lowest polarization (~ 0.3 Ω.cm2) with minimum contribution of charge transfer and concentration polarization.
In some cases this leads to significant contribution of charge transfer excitation to the absorption spectra of some chromophores while such contributions are completely absent in others.
In particular, the relative contribution of charge transfer due to surface band bending and the polarization due to molecular dipoles were determined.
The contribution of charge carrier concentration and ion mobility to the dc ionic conductivity of these composite polymeric electrolytes is discussed.
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