2008
DOI: 10.1209/0295-5075/84/57007
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Graphene as an electronic membrane

Abstract: Experiments are finally revealing intricate facts about graphene which go beyond the ideal picture of relativistic Dirac fermions in pristine two dimensional (2D) space, two years after its first isolation [1,2]. While observations of rippling [3,4,5] added another dimension to the richness of the physics of graphene, scanning single electron transistor images displayed prevalent charge inhomogeneity [6]. The importance of understanding these non-ideal aspects cannot be overstated both from the fundamental res… Show more

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Cited by 274 publications
(276 citation statements)
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“…Something similar happens for the elastic energy E el , so that the temperature derivative of the internal energy E [see Eq. (6)] also vanishes at low T . This is similar to the results of earlier path-integral simulations of 3D solids, 40,48 where the resulting data were in agreement with the basic laws of thermodynamics.…”
Section: Thermodynamic Consistencymentioning
confidence: 98%
“…Something similar happens for the elastic energy E el , so that the temperature derivative of the internal energy E [see Eq. (6)] also vanishes at low T . This is similar to the results of earlier path-integral simulations of 3D solids, 40,48 where the resulting data were in agreement with the basic laws of thermodynamics.…”
Section: Thermodynamic Consistencymentioning
confidence: 98%
“…Changes in the next-nearest-neighbour hopping also lead to an electrostatic potential V (0) that fluctuates in a randomly rippled graphene sheet (Kim Neto & Castro 2007). However, as follows from equations (3.2) and (3.3) both vector and electrostatic potentials contribute to r in a similar manner and, for brevity, we will further discuss only the effect of vector potential (4.3).…”
Section: Scattering By Ripplesmentioning
confidence: 99%
“…When graphene is grown on SiC substrate, its carrier transport is significantly affected by a range of scattering mechanisms, predominantly, long-range Coulomb scattering on charged impurities trapped in the graphene-substrate interface. Others include short-range disorder related to intrinsic lattice imperfections, point defects and dislocations, 10,11,20,22,[24][25][26][27][31][32][33][34] "ripples" in graphene's atomic structure, 6,7,[35][36][37][38] and acoustic phonons. [39][40][41] It has been calculated that in case of monolayer graphene, the room temperature intrinsic mobility of charge carriers is phononlimited to $10 5 cm 2 /Vs (Refs.…”
Section: Introductionmentioning
confidence: 99%