Abstract
The topological state that emerges at the surface of a topological insulator (TI) and at the TI-substrate interface are studied in metal–hBN–Bi2Se3 capacitors. By measuring the RF admittance of the capacitors versus gate voltage, we extract the compressibility of the Dirac state located at a gated TI surface. We show that even in the presence of an ungated surface that hosts a trivial electron accumulation layer, the other gated surface always exhibits an ambipolar effect in the quantum capacitance. We succeed in determining the velocity of surface Dirac fermions in two devices, one with a passivated surface and the other with a free surface that hosts trivial states. Our results demonstrate the potential of RF quantum capacitance techniques to probe surface states of systems in the presence of a parasitic density-of-states.
Highlights
The topological state that emerges at the surface ofa topological insulator (TI) and at the TI-substrate interface are studied in metal-hexagonal boron nitride (hBN)-Bi2Se3 capacitors
We show that even in the presence of an ungated surface that hosts a trivial electron accumulation layer, the other gated surface always exhibits an ambipolar effect in the quantum capacitance
We investigate the quantum capacitance of topological surface states and interface states in metal-insulator-topological insulator capacitor devices (MITI-CAP) having two different architectures
Summary
The topological state that emerges at the surface ofa topological insulator (TI) and at the TI-substrate interface are studied in metal-hBN-Bi2Se3 capacitors. Bi2Se3 – a prototypical topological insulator – has a large bulk energy gap (200meV) with two Dirac states bound to each surface.
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