Ersan, F.Aktürk, E.Çıracı, Salim2018-04-122018-04-122016-061932-7447http://hdl.handle.net/11693/36740Recent studies have shown that arsenic can form single-layer phases in buckled honeycomb as well as symmetric washboard structures, named as arsenene. These structures are stable even in freestanding form and are nonmagnetic semiconductors in the energy range which is suitable for various electronic applications. In this study we investigated the adsorption of selected adatoms (H, Li, B, C, N, O, Al, Si, P, Cl, Ti, Ga, Ge, As, Se, and Sb) and physisorption of molecules (H2, O2, and H2O) to these two arsene phases. Since the interaction of these adspecies with arsenene are studied using large supercells, the coupling between adspecies is minimized, and hence our results can be interpreted to mimic the effects of isolated adatom or physisorbed molecule. It is found that the adatoms form strong chemisorption bonds and hence modify the atomic structure and physical properties locally. Some of the adatoms give rise to significant local reconstruction of the atomic structure. Electronic states of some adatoms become spin polarized and attain net magnetic moments; they may even display half-metallic character at high coverage. A majority of adsorbed atoms give rise to localized states in the fundamental band gap. We showed that the interactions between H2, O2, and H2O molecules and single-layer arsenene are rather weak and do not cause any significant changes in the physical properties of these molecules, as well as those of arsenene phases. However, some of these molecules can be dissociated at the edges of the flakes of arsenene structures; their constituents are adsorbed to the edge atoms and cause local reconstructions.EnglishAdatomsAtomsElectronic statesEnergy gapGermaniumMagnetic momentsMoleculesPhysical propertiesPhysisorptionSemiconducting selenium compoundsChemisorption bondElectronic applicationFundamental band gapHalf-metallic charactersLocalized stateNon-magnetic semiconductorsPhysisorbed moleculesStructure and physical propertiesCrystal atomic structureArticle10.1021/acs.jpcc.6b02439