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Neighboring decagons must be allowed, however, to share some atoms with each other.
Two EOCs with a degree of branching of 30 and 60 hexyl side chains per 1000C atoms with each four different crosslink densities were employed.
Whereas at low pressure there are relatively few collisions of mercury atoms with each other, the collision frequency increases enormously if mercury gas is excited under high pressure (e.g., eight atmospheres or more).
Collision of the neighboring Au(0) atoms with each other lead to the formation of the AuNPs.
In Figure 1, the left and right electrodes are two semi-infinite gold leads with 3 × 3 = 9 atoms, with each layer arranged in the [111] surface geometry along the z-axis.
However, in the case of BiOCl, the salt crystal forms in a structure of alternating plates of Bi, O, and Cl atoms, with each oxygen coordinating with four bismuth atoms in the adjacent plane.
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The potential is cut off at r c =2.5a; thus, 12 neighbor shells, including a total of 248 atoms, interact with each atom.
As is the case for boranes, polycentric bonds cannot be properly represented by SMILES and bonds of the metal atom with each of the carbon atoms in a polyhapto ligand are included in our representation.
When we're dealing with atoms outside of the transition metals, we say that these orbitals form "orbital shells" around the atom, with each successive shell being further out than the ones before.
Notable features are the inclusion of the zero-order bond and the option to control the number of virtual hydrogen atoms associated with each actual atom [40].
Such orbitals result when the atomic orbitals of bonded atoms combine with each other.
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