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Solute vacancy binding energy is a key quantity in understanding solute diffusion kinetics and phase segregation, and may help choice of alloy compositions for future material design.
The interlayer binding energy is a relatively simple measure of the interlayer interactions and is defined as the energy per layer per area required separating graphite into individual graphene sheets (for example, by uniformly expanding the lattice in the direction perpendicular to the basal plane).
It is shown that the binding energy is a function of the size of dots, impurity position and external fields strength.
In general, for a fixed geometry of the unperturbed system, the exciton binding energy is a decreasing function of the intense laser field parameter and of the dc electric field, although certain combinations of the two applied field intensities may lead to a rather insensitive behavior of the binding energy with respect to the application of a dc field.
However, accurate calculation of the binding energy is a tough challenge.
Thus we can conclude that choosing the peptide template that has the lowest binding energy is a reasonable strategy.
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If P = 0, then the binding energy is an all the way decreasing function of the Al concentration.
Thus, the effects of magnetic field on the impurity binding energy are a very important problem [26 28].
The masses of chemical elements are, typically, thousands of MeV (million electron volts, in energy units), while the kinetic and binding energies are a few tens of electron volts.
This has the consequence that, even if the true binding energy is conserved, a poor method of estimating binding energies will probably assign a weaker binding energy to the S. typhimurium orthologs of those E. coli sites with the strongest estimated binding energy.
However, unlike the ground-state exciton, the first-excited binding energy is not a monotonically decreasing function of x Al 1 over the range of values of this quantity considered.
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