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      Topological invariants of eigenvalue intersections and decrease of Wannier functions in graphene

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          Abstract

          We investigate the asymptotic decrease of the Wannier functions for the valence and conduction band of graphene, both in the monolayer and the multilayer case. Since the decrease of the Wannier functions is characterised by the structure of the Bloch eigenspaces around the Dirac points, we introduce a geometric invariant of the family of eigenspaces, baptised eigenspace vorticity. We compare it with the pseudospin winding number. For every value \(n \in Z\) of the eigenspace vorticity, we exhibit a canonical model for the local topology of the eigenspaces. With the help of these canonical models, we show that the single band Wannier function \(w\) satisfies \(|w(x)| \leq \mathrm{const} |x|^{- 2}\) as \(|x| \rightarrow \infty\), both in monolayer and bilayer graphene.

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          The electronic properties of graphene

          This article reviews the basic theoretical aspects of graphene, a one atom thick allotrope of carbon, with unusual two-dimensional Dirac-like electronic excitations. The Dirac electrons can be controlled by application of external electric and magnetic fields, or by altering sample geometry and/or topology. We show that the Dirac electrons behave in unusual ways in tunneling, confinement, and integer quantum Hall effect. We discuss the electronic properties of graphene stacks and show that they vary with stacking order and number of layers. Edge (surface) states in graphene are strongly dependent on the edge termination (zigzag or armchair) and affect the physical properties of nanoribbons. We also discuss how different types of disorder modify the Dirac equation leading to unusual spectroscopic and transport properties. The effects of electron-electron and electron-phonon interactions in single layer and multilayer graphene are also presented.
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            The Band Theory of Graphite

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              \(Z_2\) Topological Order and the Quantum Spin Hall Effect

              The quantum spin Hall (QSH) phase is a time reversal invariant electronic state with a bulk electronic band gap that supports the transport of charge and spin in gapless edge states. We show that this phase is associated with a novel \(Z_2\) topological invariant, which distinguishes it from an ordinary insulator. The \(Z_2\) classification, which is defined for time reversal invariant Hamiltonians, is analogous to the Chern number classification of the quantum Hall effect. We establish the \(Z_2\) order of the QSH phase in the two band model of graphene and propose a generalization of the formalism applicable to multi band and interacting systems.
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                Author and article information

                Journal
                17 June 2013
                2014-01-16
                Article
                10.1007/s10955-014-0918-x
                1306.3904
                0f2d0a71-0e35-4fb3-967d-98f9d28bf89d

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                81Q70, 55R55, 35J10
                J. Stat. Phys. 155, 1027-1071 (2014)
                54 pages, 4 figures. Version 2: Section 1.0 added; improved results on the decay rate of Wannier functions in graphene (Th. 4.3 and Prop. 4.6). Version 3: final version, to appear in JSP. New in V3: previous Sections 3.1 and 3.2 are now Section 2.2; Lemma 2.4 modified (previous statement was not correct); major modifications to Section 2.3; Assumption 4.1(v) on the Hamiltonian changed
                math-ph cond-mat.mes-hall math.MP

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