Density dependent exchange contribution to $\partialμ/\partial n$ in extrinsic graphene

dc.creatorHwang, E. H.
dc.creatorHu, Ben Yu-Kuang
dc.creatorSarma, S. Das
dc.date2007-03-20
dc.date2007-12-03
dc.date.accessioned2026-07-07T08:46:33Z
dc.date.available2026-07-07T08:46:33Z
dc.descriptionWe calculate $\partialμ/\partial n$ in extrinsic graphene as a function of carrier density $n$ at zero temperature by obtaining the electronic self-energy within the Hartree-Fock approximation. The exchange-driven Dirac-point logarithmic singularity in the quasiparticle velocity of intrinsic graphene disappears in the extrinsic case. The calculated renormalized $\partialμ/\partial n$ in extrinsic graphene has the same qualitative $n^{-\frac12}$ density dependence as the inverse bare density of states with a 20% enhancement from the corresponding bare value, a relatively weak effect compared to the corresponding parabolic-band case.
dc.description4 pages, 3 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0703499
dc.identifierhttp://arxiv.org/abs/cond-mat/0703499
dc.identifierPhys. Rev. Lett. 99, 226801 (2007)
dc.identifierdoi:10.1103/PhysRevLett.99.226801
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/143287
dc.subjectMesoscale and Nanoscale Physics
dc.titleDensity dependent exchange contribution to $\partialμ/\partial n$ in extrinsic graphene
dc.typetext

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