General relativity and graphene

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Correction to the anomalous magnetic moment of electrons due to the defects.
Summary • Ripples occur naturally in graphene either smooth (substrate) or induced by topological defects. • Curved portions induce an effective gauge field and a space-dependent Fermi velocity. • The LDOS oscillates within regions of the ripple's size. The correlations of morphology and electronics can be observed with local probes (STM) or ARPES. • The minimal conductivity induced by topological defects depends inversely on the density of disorder • Dislocations induce an pseudovector coupling that breaks T symmetry and can have a strong influence on the physical properties (Klein paradox, weak localization). In progress.
Page 1 and 2: Evora08 General relativity and grap
Page 3 and 4: A brief history of graphene In the
Page 5 and 6: Second revolution: graphene (05) Wh
Page 7 and 8: Other interesting points of the dis
Page 9 and 10: Ripples on graphene Freely suspende
Page 11 and 12: Physical origin of the curvature
Page 13 and 14: Observation of topological defects
Page 15 and 16: Formation of topological defects Sq
Page 17 and 18: Dirac in curved space We can includ
Page 19 and 20: Multiple defects
Page 21 and 22: Cosmology versus condensed matter N
Page 23 and 24: Computation of observables Equation
Page 25 and 26: Averaging over disorder A. Cortijo
Page 27 and 28: Characterized by the Burgers vector
Page 29 and 30: Torsion in differential geometry Ba
Page 31 and 32: Dirac fermions in curved space with
Page 33: arXiv:0810.5121 Similar models. Fut
Page 37: Conclusions General relativity and

General relativity and graphene

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