Abstract

The authors perform pump-probe ARPES measurement on a SnTe (111) surface to reveal the position of the Dirac point, and the Rashba splitting of the bulk valence band.

Highlights

  • A topological crystalline insulator (TCI) has been introduced as a new class of insulators [1]

  • We have performed time-resolved ARPES (TARPES) measurement on the (111) surface of a SnTe thin film grown by molecular beam epitaxy (MBE)

  • We observed the whole structure of the surface band, having the Dirac point below the top of the bulk valence band (VB)

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Summary

Introduction

A topological crystalline insulator (TCI) has been introduced as a new class of insulators [1]. As a result of the nontrivial topology, massless spin-polarized modes emerge on the surfaces of TCI. SnTe has attracted much attention in its ferroelectric properties, because the nonpolar (centrosymmetric) rocksalt (RS) structure of the IV-VI compounds is inherently soft, or vulnerable to change into a polar (noncentrosymmetric) rhombohedral structure [5]: In the SnTe case, the structural transition was reported in bulk crystals below ∼100 K depending on the hole concentration [6,7].

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