Abstract

Topologically protected surface states present rich physics and promising spintronic, optoelectronic, and photonic applications that require a proper understanding of their ultrafast carrier dynamics. Here, we investigate these dynamics in topological insulators (TIs) of the bismuth and antimony chalcogenide family, where we isolate the response of Dirac fermions at the surface from the response of bulk carriers by combining photoexcitation with below-bandgap terahertz (THz) photons and TI samples with varying Fermi level, including one sample with the Fermi level located within the bandgap. We identify distinctly faster relaxation of charge carriers in the topologically protected Dirac surface states (few hundred femtoseconds), compared to bulk carriers (few picoseconds). In agreement with such fast cooling dynamics, we observe THz harmonic generation without any saturation effects for increasing incident fields, unlike graphene which exhibits strong saturation. This opens up promising avenues for increased THz nonlinear conversion efficiencies, and high-bandwidth optoelectronic and spintronic information and communication applications.

Highlights

  • Nowadays, due to their unique transport properties, topological insulators (TIs) attract great attention[1,2]

  • For many of these applications it is crucial to understand the characteristic timescales of the relaxation dynamics of excited carriers, and in particular determine if these dynamics are different for topological surface states compared to the bulk

  • We use THz pulses with photon energies below 4 meV, and verify whether the observed carrier dynamics originate from surface states (SSs), bulk conduction states (BCSs), or bulk valence states (BVSs), using three different TI samples with the Fermi energy in the valence band (Bi2Te3), in the conduction band (Bi2Se3), and inside the bandgap (Bi1.4Sb0.6Te1.51Se1.49, i.e. BSTS)

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Summary

Introduction

Due to their unique transport properties, topological insulators (TIs) attract great attention[1,2]. We use THz pulses with photon energies below 4 meV, and verify whether the observed carrier dynamics originate from surface states (SSs), bulk conduction states (BCSs), or bulk valence states (BVSs), using three different TI samples with the Fermi energy in the valence band (Bi2Te3), in the conduction band (Bi2Se3), and inside the bandgap (Bi1.4Sb0.6Te1.51Se1.49, i.e. BSTS).

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