In the limit of low energy, graphene can be described by a theory of free massless Fermions. In this work, we write a non-Euclidean metric that represents graphene and introduce a non-Abelian gauge field due to the presence of topological defects (disclinations). Furthermore, in this background, we study the elastic scattering of Fermions by these defects. Afterwards, we obtain the phase shift angle and the scattering amplitude. We also discuss the influence of these results to transport properties. In this approach, we apply a uniform magnetic field perpendicular to the graphene sheet. Thus, the system also becomes described by an Abelian gauge field and we observe that occurs the break of the degeneracy of Landau levels with poss...
The proposals for realizing exotic particles through coupling of quantum Hall effect to superconduct...
Because of Klein tunneling, electrostatic potentials are unable to confine Dirac electrons. We show ...
Because of Klein tunneling, electrostatic potentials are unable to confine Dirac electrons. We show ...
No limite de baixas energias, o grafeno pode ser descrito por uma teoria de férmions livres sem mass...
In this work, we study the graphene and its physical properties associated with the theory of the t...
In the past few years graphene has been shown to be an interesting object of investigation to scient...
In this work, we investigate in parallel physical and mathematical aspects inherent to the problem ...
In this work, we investigate in parallel physical and mathematical aspects inherent to the problem ...
In this article we employ a simple nonrelativistic model to describe the low energy excitation of gr...
Graphene is a two-dimensional carbon allotrope with a honeycomb crystal structure in which electroni...
The Graphene is a two-dimensional(2-D) semiconductor crystal with null gap, where charge carriers b...
The Graphene is a two-dimensional(2-D) semiconductor crystal with null gap, where charge carriers b...
Esse trabalho e dedicado ao estudo de transporte eletrônico em sistemas quânticos de baixa dimensi...
Graphene is a two dimensional material made of single layer of carbon atoms arranging into a honeyc...
In this work, we study the low-energy electronic spectrum of a graphene layer structure with a discl...
The proposals for realizing exotic particles through coupling of quantum Hall effect to superconduct...
Because of Klein tunneling, electrostatic potentials are unable to confine Dirac electrons. We show ...
Because of Klein tunneling, electrostatic potentials are unable to confine Dirac electrons. We show ...
No limite de baixas energias, o grafeno pode ser descrito por uma teoria de férmions livres sem mass...
In this work, we study the graphene and its physical properties associated with the theory of the t...
In the past few years graphene has been shown to be an interesting object of investigation to scient...
In this work, we investigate in parallel physical and mathematical aspects inherent to the problem ...
In this work, we investigate in parallel physical and mathematical aspects inherent to the problem ...
In this article we employ a simple nonrelativistic model to describe the low energy excitation of gr...
Graphene is a two-dimensional carbon allotrope with a honeycomb crystal structure in which electroni...
The Graphene is a two-dimensional(2-D) semiconductor crystal with null gap, where charge carriers b...
The Graphene is a two-dimensional(2-D) semiconductor crystal with null gap, where charge carriers b...
Esse trabalho e dedicado ao estudo de transporte eletrônico em sistemas quânticos de baixa dimensi...
Graphene is a two dimensional material made of single layer of carbon atoms arranging into a honeyc...
In this work, we study the low-energy electronic spectrum of a graphene layer structure with a discl...
The proposals for realizing exotic particles through coupling of quantum Hall effect to superconduct...
Because of Klein tunneling, electrostatic potentials are unable to confine Dirac electrons. We show ...
Because of Klein tunneling, electrostatic potentials are unable to confine Dirac electrons. We show ...