Author
Listed:
- Tay-Rong Chang
(National Tsing Hua University)
- Su-Yang Xu
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University)
- Guoqing Chang
(Centre for Advanced 2D Materials and Graphene Research Centre, National University of Singapore
National University of Singapore)
- Chi-Cheng Lee
(Centre for Advanced 2D Materials and Graphene Research Centre, National University of Singapore
National University of Singapore)
- Shin-Ming Huang
(Centre for Advanced 2D Materials and Graphene Research Centre, National University of Singapore
National University of Singapore)
- BaoKai Wang
(Centre for Advanced 2D Materials and Graphene Research Centre, National University of Singapore
National University of Singapore
Northeastern University)
- Guang Bian
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University)
- Hao Zheng
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University)
- Daniel S. Sanchez
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University)
- Ilya Belopolski
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University)
- Nasser Alidoust
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University)
- Madhab Neupane
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University
Condensed Matter and Magnet Science Group, Los Alamos National Laboratory)
- Arun Bansil
(Northeastern University)
- Horng-Tay Jeng
(National Tsing Hua University
Institute of Physics, Academia Sinica)
- Hsin Lin
(Centre for Advanced 2D Materials and Graphene Research Centre, National University of Singapore
National University of Singapore)
- M. Zahid Hasan
(Laboratory for Topological Quantum Matter and Spectroscopy (B7), Princeton University
Princeton Center for Complex Materials, Princeton Institute for the Science and Technology of Materials, Princeton University)
Abstract
A Weyl semimetal is a new state of matter that hosts Weyl fermions as emergent quasiparticles. The Weyl fermions correspond to isolated points of bulk band degeneracy, Weyl nodes, which are connected only through the crystal’s boundary by exotic Fermi arcs. The length of the Fermi arc gives a measure of the topological strength, because the only way to destroy the Weyl nodes is to annihilate them in pairs in the reciprocal space. To date, Weyl semimetals are only realized in the TaAs class. Here, we propose a tunable Weyl state in MoxW1−xTe2 where Weyl nodes are formed by touching points between metallic pockets. We show that the Fermi arc length can be changed as a function of Mo concentration, thus tuning the topological strength. Our results provide an experimentally feasible route to realizing Weyl physics in the layered compound MoxW1−xTe2, where non-saturating magneto-resistance and pressure-driven superconductivity have been observed.
Suggested Citation
Tay-Rong Chang & Su-Yang Xu & Guoqing Chang & Chi-Cheng Lee & Shin-Ming Huang & BaoKai Wang & Guang Bian & Hao Zheng & Daniel S. Sanchez & Ilya Belopolski & Nasser Alidoust & Madhab Neupane & Arun Ban, 2016.
"Prediction of an arc-tunable Weyl Fermion metallic state in MoxW1−xTe2,"
Nature Communications, Nature, vol. 7(1), pages 1-9, April.
Handle:
RePEc:nat:natcom:v:7:y:2016:i:1:d:10.1038_ncomms10639
DOI: 10.1038/ncomms10639
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