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Depth-resolved SHG measurements conducted in the LiTaO3 bulk crystal show that the Bloch-type walls are stable across the crystal depth.
1P-TRPL on the Cd-treated CdTe crystal show a slow lifetime component of 5 ns, which is a factor of >10× lower than the bulk lifetime measured using 2P-TRPL (5 ns vs. >70 ns).
Dislocation dynamic simulations in a face-centered cubic crystal show these three types of behavior and give the conditions under which a dissociated dislocation can move through a channel bordered by impenetrable obstacles.
Analyses of the Tm3+ lifetime data for the co-doped crystal show that the energy transfer processes from the Tm3+ sensitizers to the Pr3+ acceptors have high quantum efficiencies.
The two independent Spy0129 molecules in the crystal show differences in the positions and orientations of the catalytic Cys and His residues, Cys221 and His126, correlated with movements of the β7/β8 and β4/β5 loops that respectively follow these residues.
The results for the naphthalene crystal show quick convergence of the non-local energy as a function of the integration volume.
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X-ray diffraction (XRD) on a single crystal showed that the latter was crystallized in P-1 space group.
(b) Illustration of the three-dimensional geometry for the ice crystal shown in (a).
Finally, the crystal shows two K+ binding sites per subunit.
The switching effect observed in such crystal shows memory.
Figure 1(b) shows the three-dimensional geometry of the ice crystal shown in Fig. 1(a).
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CEO of Professional Science Editing for Scientists @ prosciediting.com