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The Barlow packings consist of translated planes (layers) of contacting spheres with centers arranged on the sites of a triangular lattice, where the layers are stacked on top of one another. In the stackings, there are three possible translations relative to the central layer (the layer including the central sphere), denoted A, B, and C, obeying the rule that no layer can be consecutively repeated. We have found that it is only the positions of the A layers relative to the central layer that are relevant in determining the coordination shells about the central sphere. The fcc Barlow stacking, denoted by repeating ABC layers, is, thus, indistinguishable to the similarity metric from any other stacking with an A layer repeated every three layers
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In the diagrams of paper I, e.g., for DLP optimal packings in R2 for N=24, N=45, and N=95 disks, it is difficult to perceive that the disks forming a cavity around the central disk are not all the same radial distance from the central disk. However, although the difference in radial distances between these disks is small, it is far larger than the precision to which the spatial positions of sphere centers are calculated by the algorithm
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