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3.4 Existence of Super‐Structural Units

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In B2O3 glass the presence of rigid, planar boroxol B3O6 units made up of three trigonal BO3 units is well established [20]. In contrast to basic polyhedral units, ABV, where a single A atom is coordinated by B atoms, super‐structural units such as boroxol units contain more than one A atom. Do super‐structural units then exist in other borate glasses? It is a question that has long persisted in the oxide‐glass science.

Super‐structural units may be energetically more favorable in systems with long‐range interactions. However, their larger size raises difficulties to match the density of networks with the observed density of glass. For example, the boroxol units are topologically equivalent to the basic BO3 trigonal unit (both have δ = 2 and V = 3). If all BO3 trigonal units in B2O3 glass are replaced by B3O6 boroxol units, the length scale of the structural unit is doubled (the volume thus increasing by a factor of 8) while the mass of the unit is only tripled so that the density of a network of boroxol units is only 3/8 of that of a network of trigonal units. Further, based on topological considerations mentioned before, an extended 3‐D network can incorporate only a small fraction of super‐structural units with V > 4. For this reason, the di‐pentaborate and the di‐triborate groups, two of the six super‐structural units listed by Wright [20], probably do not exist in significant concentrations.

Encyclopedia of Glass Science, Technology, History, and Culture

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