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Additional info for DESERFEST A Celebration of the Life and Works of Stanley Deser Michigan Center for Theoretical Physics, University of Michigan, Ann Arbor, USA, 3 – 5 April 2004
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L. G. Louie, Nat. Phys. 4, 213 (2008) 1 Experimental Manifestation of Berry Phase in Graphene 27 109. P. Bliokh, V. Freilikher, S. Savelev, F. Nori, Phys. Rev. B 79, 075123 (2009) 110. -H. -W. Son, L. L. G. Louie, Phys. Rev. Lett. 103, 046808 (2009) 111. N. Abedpour, A. Esmailpour, R. R. Tabar, Phys. Rev. B 79, 165412 (2009) 112. M. M. Peeters, P. M. Pereira, Phys. Rev. B 77, 115446 (2008) 113. J. Milton Pereira, P. M. Peeters, Appl. Phys. Lett. 90, 132122 (2007) Chapter 2 Probing Dirac Fermions in Graphene by Scanning Tunneling Microscopy and Spectroscopy Adina Luican-Mayer and Eva Y.
In a realistic situation the measurement temperature imposes a lower bound on the resolution which cannot be better than the thermal broadening: E ≈ kT . 35 meV. At the same time the ac. bias modulation should be comparable to this value for optimal resolution. Furthermore, common materials used for the tip such as Pt/Ir, W, Au typically satisfy the condition of a flat DOS for small enough voltages. For a reliable STS measurement one needs to check that the experiment is done in the vacuum tunneling regime when the dependence of the tunneling current on tip-sample distance is exponential [4].
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