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1.
J Phys Condens Matter ; 29(4): 045302, 2017 Feb 01.
Article in English | MEDLINE | ID: mdl-27882899

ABSTRACT

We use first-principles simulations to investigate the topological properties of Bi2Se3 thin films deposited on amorphous SiO2, Bi2Se3/a-SiO2, which is a promising substrate for topological insulator (TI) based device applications. The Bi2Se3 films are bonded to a-SiO2 mediated by van der Waals interactions. Upon interaction with the substrate, the Bi2Se3 topological surface and interface states remain present, however the degeneracy between the Dirac-like cones is broken. The energy separation between the two Dirac-like cones increases with the number of Bi2Se3 quintuple layers (QLs) deposited on the substrate. Such a degeneracy breaking is caused by (i) charge transfer from the TI to the substrate and charge redistribution along the Bi2Se3 QLs, and (ii) by deformation of the QL in contact with the a-SiO2 substrate. We also investigate the role played by oxygen vacancies ([Formula: see text]) on the a-SiO2, which increases the energy splitting between the two Dirac-like cones. Finally, by mapping the electronic structure of Bi2Se3/a-SiO2, we found that the a-SiO2 surface states, even upon the presence of [Formula: see text], play a minor role on gating the electronic transport properties of Bi2Se3.

2.
J Phys Condens Matter ; 25(44): 445301, 2013 Nov 06.
Article in English | MEDLINE | ID: mdl-24113295

ABSTRACT

Based on ab initio calculations, we examine the incorporation of Li atoms in the MoS2/graphene interface. We find that the intercalated Li atoms are energetically more stable than Li atoms adsorbed on the MoS2 surface. The intercalated atoms interact with both graphene sheet and MoS2 layer, increasing the Li binding energies. However, the equilibrium geometries are ruled by the MoS2 layer, where the intercalated Li atoms lie on the top (LiT) and hollow (LiH) sites of the MoS2 layer. We calculate the Li diffusion barriers, along the LiT → LiH diffusion path, where we find similar energy barriers compared with that obtained for Li adatoms on the MoS2 surface. Our results allow us to infer that the Li storage capacity increases at MoS2/G interfaces, in comparison with Li adatoms on the MoS2 surface-however, with no reduction on the mobility of the intercalated Li atoms. Those properties are interesting/useful to the development of Li batteries based on MoS2.

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