Abstract

We demonstrate experimentally that graphene quantum capacitance CqC_{\mathrm{q}} can have a strong impact on transport spectroscopy through the interplay with nearby charge reservoirs. The effect is elucidated in a field-effect-gated epitaxial graphene device, in which interface states serve as charge reservoirs. The Fermi-level dependence of CqC_{\mathrm{q}} is manifested as an unusual parabolic gate voltage (VgV_{\mathrm{g}}) dependence of the carrier density, centered on the Dirac point. Consequently, in high magnetic fields BB, the spectroscopy of longitudinal resistance (RxxR_{xx}) vs. VgV_{\mathrm{g}} represents the structure of the unequally spaced relativistic graphene Landau levels (LLs). RxxR_{xx} mapping vs. VgV_{\mathrm{g}} and BB thus reveals the vital role of the zero-energy LL on the development of the anomalously wide ν=2ν=2 quantum Hall state.

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