Abstract

The weak intrinsic spin-orbit coupling in graphene can be greatly enhanced by proximity coupling. Here we report on the proximity-induced spin-orbit coupling in graphene transferred by hexagonal boron nitride (hBN) onto the topological insulator Bi$_{1.5}$Sb$_{0.5}$Te$_{1.7}$Se$_{1.3}$ (BSTS) which was grown on a hBN substrate by vapor solid synthesis. Phase coherent transport measurements, revealing weak localization, allow us to extract the carrier density-dependent phase coherence length $l_\phi$. While $l_\phi$ increases with increasing carrier density in the hBN/graphene/hBN reference sample, it decreases in BSTS/graphene due to the proximity-coupling of BSTS to graphene. The latter behavior results from D'yakonov-Perel-type spin scattering in graphene with a large proximity-induced spin-orbit coupling strength of at least 2.5 meV.

Highlights

  • The weak intrinsic spin-orbit coupling in graphene can be greatly enhanced by proximity coupling

  • We report on the proximity-induced spin-orbit coupling in graphene transferred by hexagonal boron nitride onto the topological insulator Bi1.5Sb0.5Te1.7Se1.3 (BSTS) which was grown on a hBN substrate by vapor solid synthesis

  • While lφ increases with increasing carrier density in the hBN/graphene/hBN reference sample, it decreases in graphene/BSTS due to the proximity-coupling of BSTS to graphene

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Summary

Introduction

The weak intrinsic spin-orbit coupling in graphene can be greatly enhanced by proximity coupling. This is the accepted version of the article: Jafarpisheh S., Cummings A.W., Watanabe K., Taniguchi T., Beschoten B., Stampfer C..

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