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Although a single positive charge thus made a major contribution to binding energy, we found that a second, immediately adjacent, positive charge, here exemplified by an α-amino group, added significantly to overall affinity for each of the four CR domains, so that such pairs of positive charges are likely to be highly preferred binding loci on protein ligands compared with single lysine residues.
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Based on a stability analysis of the H binding energies, we find that the largest H solute defect complex for V, Cr, Co, Ni and Zn contains two H atoms, while for Sc, Ti, Mn, and Cu the largest defect complex contains four H atoms.
With the same binding energy cutoff, we found two human miRNAs hsa-miR-370 and hsa-miR-661 having MREs within NS1 genes of all types of dengue virus.
The total binding energy is found to increase with increasing glyme length and follows: NH>O>S.
A significant shift in binding energy was found in Pt NPs deposited on NMC with disordered pore structure compared to Pt NPs deposited on NMC with ordered pore structure.
The wave functions and polaron binding energy are found.
The polaron binding energy is found by substitution of Eq. 27 to 26: (26).
The average surface binding energy was found at the same value of 3.1 eV irrespective to the used density of Ag (Fig. 6 a, b).
Importantly, the free binding energy computed was found to have high quantitative correlation (R2 ∼ 95%) with experimental results.
Relative intensities of the core level photoelectron peaks and their chemical shifts derived from binding energy changes are found to give precise information on physico-chemical properties and quality of the buried layers.
For samples without thiol-functionalization, no binding energy peak was found.
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