Author
Listed:
- Frank Arnold
(Max Planck Institute for Chemical Physics of Solids)
- Chandra Shekhar
(Max Planck Institute for Chemical Physics of Solids)
- Shu-Chun Wu
(Max Planck Institute for Chemical Physics of Solids)
- Yan Sun
(Max Planck Institute for Chemical Physics of Solids)
- Ricardo Donizeth dos Reis
(Max Planck Institute for Chemical Physics of Solids)
- Nitesh Kumar
(Max Planck Institute for Chemical Physics of Solids)
- Marcel Naumann
(Max Planck Institute for Chemical Physics of Solids)
- Mukkattu O. Ajeesh
(Max Planck Institute for Chemical Physics of Solids)
- Marcus Schmidt
(Max Planck Institute for Chemical Physics of Solids)
- Adolfo G. Grushin
(Max Planck Institute for the Physics of Complex Systems)
- Jens H. Bardarson
(Max Planck Institute for the Physics of Complex Systems)
- Michael Baenitz
(Max Planck Institute for Chemical Physics of Solids)
- Dmitry Sokolov
(Max Planck Institute for Chemical Physics of Solids)
- Horst Borrmann
(Max Planck Institute for Chemical Physics of Solids)
- Michael Nicklas
(Max Planck Institute for Chemical Physics of Solids)
- Claudia Felser
(Max Planck Institute for Chemical Physics of Solids)
- Elena Hassinger
(Max Planck Institute for Chemical Physics of Solids)
- Binghai Yan
(Max Planck Institute for Chemical Physics of Solids
Max Planck Institute for the Physics of Complex Systems)
Abstract
Weyl semimetals (WSMs) are topological quantum states wherein the electronic bands disperse linearly around pairs of nodes with fixed chirality, the Weyl points. In WSMs, nonorthogonal electric and magnetic fields induce an exotic phenomenon known as the chiral anomaly, resulting in an unconventional negative longitudinal magnetoresistance, the chiral-magnetic effect. However, it remains an open question to which extent this effect survives when chirality is not well-defined. Here, we establish the detailed Fermi-surface topology of the recently identified WSM TaP via combined angle-resolved quantum-oscillation spectra and band-structure calculations. The Fermi surface forms banana-shaped electron and hole pockets surrounding pairs of Weyl points. Although this means that chirality is ill-defined in TaP, we observe a large negative longitudinal magnetoresistance. We show that the magnetoresistance can be affected by a magnetic field-induced inhomogeneous current distribution inside the sample.
Suggested Citation
Frank Arnold & Chandra Shekhar & Shu-Chun Wu & Yan Sun & Ricardo Donizeth dos Reis & Nitesh Kumar & Marcel Naumann & Mukkattu O. Ajeesh & Marcus Schmidt & Adolfo G. Grushin & Jens H. Bardarson & Micha, 2016.
"Negative magnetoresistance without well-defined chirality in the Weyl semimetal TaP,"
Nature Communications, Nature, vol. 7(1), pages 1-7, September.
Handle:
RePEc:nat:natcom:v:7:y:2016:i:1:d:10.1038_ncomms11615
DOI: 10.1038/ncomms11615
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Cited by:
- Xinjian Wei & Congkuan Tian & Hang Cui & Yuxin Zhai & Yongkai Li & Shaobo Liu & Yuanjun Song & Ya Feng & Miaoling Huang & Zhiwei Wang & Yi Liu & Qihua Xiong & Yugui Yao & X. C. Xie & Jian-Hao Chen, 2024.
"Three-dimensional hidden phase probed by in-plane magnetotransport in kagome metal CsV3Sb5 thin flakes,"
Nature Communications, Nature, vol. 15(1), pages 1-8, December.
- Lorenzo Rocchino & Federico Balduini & Heinz Schmid & Alan Molinari & Mathieu Luisier & Vicky Süß & Claudia Felser & Bernd Gotsmann & Cezar B. Zota, 2024.
"Magnetoresistive-coupled transistor using the Weyl semimetal NbP,"
Nature Communications, Nature, vol. 15(1), pages 1-8, December.
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