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High Positive MR and Energy Band Structure of RuSb(2+)

A high positive magnetoresistance (MR), 78%, is observed at 2 K on the ab plane of the diamagnetic RuSb(2+) semiconductor. On the ac plane, MR is 44% at 2 K, and about 7% at 300 K. MR at different temperatures do not follow the Kohler’s rule. It suggests that the multiband effect plays a role on the...

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Detalles Bibliográficos
Autores principales: Zhang, Liang, Wang, Yun, Chang, Hong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7412452/
https://www.ncbi.nlm.nih.gov/pubmed/32679843
http://dx.doi.org/10.3390/ma13143159
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author Zhang, Liang
Wang, Yun
Chang, Hong
author_facet Zhang, Liang
Wang, Yun
Chang, Hong
author_sort Zhang, Liang
collection PubMed
description A high positive magnetoresistance (MR), 78%, is observed at 2 K on the ab plane of the diamagnetic RuSb(2+) semiconductor. On the ac plane, MR is 44% at 2 K, and about 7% at 300 K. MR at different temperatures do not follow the Kohler’s rule. It suggests that the multiband effect plays a role on the carrier transportation. RuSb(2+) is a semiconductor with both positive and negative carriers. The quantum interference effect with the weak localization correction lies behind the high positive MR at low temperature. Judged from the ultraviolet–visible spectra, it has a direct band gap of 1.29 eV. The valence band is 0.39 eV below the Fermi energy. The schematic energy band structure is proposed based on experimental results.
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spelling pubmed-74124522020-08-26 High Positive MR and Energy Band Structure of RuSb(2+) Zhang, Liang Wang, Yun Chang, Hong Materials (Basel) Article A high positive magnetoresistance (MR), 78%, is observed at 2 K on the ab plane of the diamagnetic RuSb(2+) semiconductor. On the ac plane, MR is 44% at 2 K, and about 7% at 300 K. MR at different temperatures do not follow the Kohler’s rule. It suggests that the multiband effect plays a role on the carrier transportation. RuSb(2+) is a semiconductor with both positive and negative carriers. The quantum interference effect with the weak localization correction lies behind the high positive MR at low temperature. Judged from the ultraviolet–visible spectra, it has a direct band gap of 1.29 eV. The valence band is 0.39 eV below the Fermi energy. The schematic energy band structure is proposed based on experimental results. MDPI 2020-07-15 /pmc/articles/PMC7412452/ /pubmed/32679843 http://dx.doi.org/10.3390/ma13143159 Text en © 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Zhang, Liang
Wang, Yun
Chang, Hong
High Positive MR and Energy Band Structure of RuSb(2+)
title High Positive MR and Energy Band Structure of RuSb(2+)
title_full High Positive MR and Energy Band Structure of RuSb(2+)
title_fullStr High Positive MR and Energy Band Structure of RuSb(2+)
title_full_unstemmed High Positive MR and Energy Band Structure of RuSb(2+)
title_short High Positive MR and Energy Band Structure of RuSb(2+)
title_sort high positive mr and energy band structure of rusb(2+)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7412452/
https://www.ncbi.nlm.nih.gov/pubmed/32679843
http://dx.doi.org/10.3390/ma13143159
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