“…Recently, the synthesis of this 2D nonhexagonal, monolayer structure (which consists of the adjacent octagon- ( o ), hexagon- ( h ), and square- ( s ) rings and is specified briefly as C ohs structure in this text) have been realized using different processes. , Even if the 3-fold coordination of atoms is maintained in this new allotrope, the sp 2 -hybridization is deformed. Very recently, we showed that not only the C ohs structure, but also stable ohs monolayers of other group IV elements (Si, Ge), group IV–IV (SiC, GeC, SnC), III–V (BN, BP, BAs, BSb, AlN, AlP, GaN, InN), and II–VI (ZnSe) compounds and their multilayers, as well as 3D periodic ohs crystals, can be regarded a new class of materials like their counterparts in the honeycomb network. − Here, C, Si, and Ge ohs monolayers of group IV elements have been found to be good metals as a consequence of multiple crossing of the Fermi level by p z -bands, in contrast to their Dirac semimetal counterparts in a honeycomb network, namely graphene, silicene, and germanene. − Recent studies on the adsorption of adatoms like H, O, C, Si, F, Ti, and Gd on bare C ohs monolayer have predicted various critical effects on the electronic properties. − In particular, it has been demonstrated that C and Si ohs monolayers can acquire novel magnetic and electronic states. These functional properties are tunable by the coverage of diverse adatoms, by the formation of vacancy and other point defects .…”