Helical quantum Hall phase in graphene on SrTiO 3

Author:

Veyrat Louis1ORCID,Déprez Corentin1,Coissard Alexis1,Li Xiaoxi234ORCID,Gay Frédéric1ORCID,Watanabe Kenji5ORCID,Taniguchi Takashi5,Han Zheng234ORCID,Piot Benjamin A.6,Sellier Hermann1ORCID,Sacépé Benjamin1ORCID

Affiliation:

1. Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, 38000 Grenoble, France.

2. Shenyang National Laboratory for Materials Science, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, P. R. China.

3. School of Material Science and Engineering, University of Science and Technology of China, Anhui 230026, P. R. China.

4. State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan 030006, P. R. China.

5. National Institute for Materials Science, 1-1 Namiki, Tsukuba 306-0044, Japan.

6. Université Grenoble Alpes, UPS-INSA-EMFL-CNRS-LNCMI, 38000 Grenoble, France.

Abstract

Controlling the interactions Near charge neutrality and subject to perpendicular magnetic fields, graphene is expected to become a ferromagnet with edge states not unlike those in two-dimensional topological insulators. Observing this effect experimentally has proven tricky because very large magnetic fields are needed to overcome the effect of electron-electron interactions, which drive the system to competing states. Instead of amping up the field, Veyrat et al. placed their graphene samples on a substrate made out of strontium titanate, which effectively screened the interactions. Transport measurements confirmed the formation of the characteristic edge states. Science , this issue p. 781

Funder

H2020 European Research Council

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

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