“…In general, one can classify the alloys into three main classes: (i) those which possess a bowing character such as the common-cation CdSe x Te 1−x and ZnSe x Te 1−x alloys [3][4][5][6][7][8]; (ii) those which possess almost a linear variation of bandgap energy versus composition such as the common-anion Cd 1−x Zn x Se and Cd 1−x Zn x Te alloys [6][7][8][9]; (iii) Those which neither have the bowing nor the linear behaviors, such as, the metallization observed in the highly lattice mismatched nitride IIIV 1−x N x alloys [10][11][12][13][14], the negative bowing behavior seen in the alloys of In x Ga 1−x As [15] and GaSb x As 1−x [16], and the anomalous behavior in lead chalcogenides [17] where the direct gap is measured to be at the L point of the Brillouin zone. Nevertheless, despite decades of extensive studies, there is no commonly accepted explanation for the different characters of bandgap variation as a function of alloy composition.…”