Dirac cones reshaped by interaction effects in suspended graphene
D. C. Elias, R. V. Gorbachev, A. S. Mayorov, S. V. Morozov, A. A., Zhukov, P. Blake, L. A. Ponomarenko, I. V. Grigorieva, K. S. Novoselov, F., Guinea, A. K. Geim

TL;DR
This study measures the cyclotron mass in suspended graphene, revealing that electron-electron interactions significantly modify the Dirac spectrum and increase the Fermi velocity at low carrier concentrations, challenging the single-particle model.
Contribution
It provides experimental evidence of interaction-induced renormalization of the Dirac cones in graphene, showing a substantial increase in Fermi velocity at low densities.
Findings
Fermi velocity reaches ~3x10^6 m/s at low carrier density
Electron-electron interactions cause nonlinear spectral behavior
Upper limit of ~0.1 meV on possible energy gap in graphene
Abstract
We report measurements of the cyclotron mass in graphene for carrier concentrations n varying over three orders of magnitude. In contrast to the single-particle picture, the real spectrum of graphene is profoundly nonlinear so that the Fermi velocity describing the spectral slope reaches ~3x10^6 m/s at n <10^10 cm^-2, three times the value commonly used for graphene. The observed changes are attributed to electron-electron interaction that renormalizes the Dirac spectrum because of weak screening. Our experiments also put an upper limit of ~0.1 meV on the possible gap in graphene.
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