Electronic properties of curved few-layers graphene : a geometrical approach.

We show the presence of non-relativistic Lévy-Leblond fermions in flat three- and four-layers graphene with AB stacking, extending the results obtained in Cariglia et al. 2017 for bilayer graphene. When the layer is curved we obtain a set of equations for Galilean fermions that are a variation of th...

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Bibliographic Details
Authors: Cariglia, Marco, Giambò, Roberto, Perali, Andrea
Format: article
Status:Published version
Publication Date:2018
Country:Brasil
Institution:Universidade Federal de Ouro Preto (UFOP)
Repository:Repositório Institucional da UFOP
Language:English
OAI Identifier:oai:repositorio.ufop.br:123456789/10471
Online Access:http://www.repositorio.ufop.br/handle/123456789/10471
Access Level:Open access
Keyword:Lévy-Leblond equations
Non-relativistic fermions
Eisenhart lift
Curved systems
Description
Summary:We show the presence of non-relativistic Lévy-Leblond fermions in flat three- and four-layers graphene with AB stacking, extending the results obtained in Cariglia et al. 2017 for bilayer graphene. When the layer is curved we obtain a set of equations for Galilean fermions that are a variation of those of Lévy-Leblond with a well defined combination of pseudospin, and that admit Lévy-Leblond spinors as solutions in an approriate limit. The local energy of such Galilean fermions is sensitive to the intrinsic curvature of the surface. We discuss the relationship between two-dimensional pseudospin, labelling layer degrees of freedom, and the different energy bands. For Lévy-Leblond fermions, an interpretation is given in terms of massless fermions in an effective 4D spacetime, and in this case the pseudospin is related to four dimensional chirality. A non-zero energy band gap between conduction and valence electronic bands is obtained for surfaces with positive curvature.