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Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal
Although, the long-standing debate on the resistivity anomaly in ZrTe(5) somewhat comes to an end, the exact topological nature of the electronic band structure remains elusive till today. Theoretical calculations predicted that bulk ZrTe(5) to be either a weak or a strong three-dimensional (3D) top...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5220326/ https://www.ncbi.nlm.nih.gov/pubmed/28067306 http://dx.doi.org/10.1038/srep40327 |
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author | Pariari, Arnab Mandal, Prabhat |
author_facet | Pariari, Arnab Mandal, Prabhat |
author_sort | Pariari, Arnab |
collection | PubMed |
description | Although, the long-standing debate on the resistivity anomaly in ZrTe(5) somewhat comes to an end, the exact topological nature of the electronic band structure remains elusive till today. Theoretical calculations predicted that bulk ZrTe(5) to be either a weak or a strong three-dimensional (3D) topological insulator. However, the angle resolved photoemission spectroscopy and transport measurements clearly demonstrate 3D Dirac cone state with a small mass gap between the valence band and conduction band in the bulk. From the magnetization and magneto-transport measurements on ZrTe(5) single crystal, we have detected both the signature of helical spin texture from topological surface state and chiral anomaly associated with the 3D Dirac cone state in the bulk. This implies that ZrTe(5) hosts a novel electronic phase of material, having massless Dirac fermionic excitation in its bulk gap state, unlike earlier reported 3D topological insulators. Apart from the band topology, it is also apparent from the resistivity and Hall measurements that the anomalous peak in the resistivity can be shifted to a much lower temperature (T < 2 K) by controlling impurity and defects. |
format | Online Article Text |
id | pubmed-5220326 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-52203262017-01-11 Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal Pariari, Arnab Mandal, Prabhat Sci Rep Article Although, the long-standing debate on the resistivity anomaly in ZrTe(5) somewhat comes to an end, the exact topological nature of the electronic band structure remains elusive till today. Theoretical calculations predicted that bulk ZrTe(5) to be either a weak or a strong three-dimensional (3D) topological insulator. However, the angle resolved photoemission spectroscopy and transport measurements clearly demonstrate 3D Dirac cone state with a small mass gap between the valence band and conduction band in the bulk. From the magnetization and magneto-transport measurements on ZrTe(5) single crystal, we have detected both the signature of helical spin texture from topological surface state and chiral anomaly associated with the 3D Dirac cone state in the bulk. This implies that ZrTe(5) hosts a novel electronic phase of material, having massless Dirac fermionic excitation in its bulk gap state, unlike earlier reported 3D topological insulators. Apart from the band topology, it is also apparent from the resistivity and Hall measurements that the anomalous peak in the resistivity can be shifted to a much lower temperature (T < 2 K) by controlling impurity and defects. Nature Publishing Group 2017-01-09 /pmc/articles/PMC5220326/ /pubmed/28067306 http://dx.doi.org/10.1038/srep40327 Text en Copyright © 2017, The Author(s) http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Pariari, Arnab Mandal, Prabhat Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal |
title | Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal |
title_full | Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal |
title_fullStr | Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal |
title_full_unstemmed | Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal |
title_short | Coexistence of topological Dirac fermions on the surface and three-dimensional Dirac cone state in the bulk of ZrTe(5) single crystal |
title_sort | coexistence of topological dirac fermions on the surface and three-dimensional dirac cone state in the bulk of zrte(5) single crystal |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5220326/ https://www.ncbi.nlm.nih.gov/pubmed/28067306 http://dx.doi.org/10.1038/srep40327 |
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