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Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni)
In this work, we investigated the phase transition and electronic structures of some newly designed all-d-metal Heusler compounds, X(2)MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni), by means of the first principles. The competition between the XA and L2(1) structures of these materials was studied, and we f...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Frontiers Media S.A.
2020
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7759634/ https://www.ncbi.nlm.nih.gov/pubmed/33363101 http://dx.doi.org/10.3389/fchem.2020.546947 |
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author | Wu, Mengxin Zhou, Feng Khenata, Rabah Kuang, Minquan Wang, Xiaotian |
author_facet | Wu, Mengxin Zhou, Feng Khenata, Rabah Kuang, Minquan Wang, Xiaotian |
author_sort | Wu, Mengxin |
collection | PubMed |
description | In this work, we investigated the phase transition and electronic structures of some newly designed all-d-metal Heusler compounds, X(2)MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni), by means of the first principles. The competition between the XA and L2(1) structures of these materials was studied, and we found that X(2)MnTi favors to feature the L2(1)-type structure, which is consistent with the well-known site-preference rule (SPR). Under the L2(1) structure, we have studied the most stable magnetic state of these materials, and we found that the ferromagnetic state is the most stable due to its lower energy. Through tetragonal deformation, we found that the L2(1) structure is no longer the most stable structure, and a more stable tetragonal L1(0) structure appeared. That is, under the tetragonal strain, the material enjoys a tetragonal phase transformation (i.e., from cubic L2(1) to tetragonal L1(0) structure). This mechanism of L2(1)-L1(0) structure transition is discussed in detail based on the calculated density of states. Moreover, we found that the energy difference between the most stable phases of L1(0) and L2(1), defined as ΔE(M) (ΔE(M) = E(Cubic)-E(Tetragonal)), can be adjusted by the uniform strain. Finally, the phonon spectra of all tetragonal X(2)MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni) phases are exhibited, which provides a powerful evidence for the stability of the tetragonal L1(0) state. We hope that our research can provide a theoretical guidance for future experimental investigations. |
format | Online Article Text |
id | pubmed-7759634 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Frontiers Media S.A. |
record_format | MEDLINE/PubMed |
spelling | pubmed-77596342020-12-26 Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni) Wu, Mengxin Zhou, Feng Khenata, Rabah Kuang, Minquan Wang, Xiaotian Front Chem Chemistry In this work, we investigated the phase transition and electronic structures of some newly designed all-d-metal Heusler compounds, X(2)MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni), by means of the first principles. The competition between the XA and L2(1) structures of these materials was studied, and we found that X(2)MnTi favors to feature the L2(1)-type structure, which is consistent with the well-known site-preference rule (SPR). Under the L2(1) structure, we have studied the most stable magnetic state of these materials, and we found that the ferromagnetic state is the most stable due to its lower energy. Through tetragonal deformation, we found that the L2(1) structure is no longer the most stable structure, and a more stable tetragonal L1(0) structure appeared. That is, under the tetragonal strain, the material enjoys a tetragonal phase transformation (i.e., from cubic L2(1) to tetragonal L1(0) structure). This mechanism of L2(1)-L1(0) structure transition is discussed in detail based on the calculated density of states. Moreover, we found that the energy difference between the most stable phases of L1(0) and L2(1), defined as ΔE(M) (ΔE(M) = E(Cubic)-E(Tetragonal)), can be adjusted by the uniform strain. Finally, the phonon spectra of all tetragonal X(2)MnTi (X = Pd, Pt, Ag, Au, Cu, and Ni) phases are exhibited, which provides a powerful evidence for the stability of the tetragonal L1(0) state. We hope that our research can provide a theoretical guidance for future experimental investigations. Frontiers Media S.A. 2020-12-11 /pmc/articles/PMC7759634/ /pubmed/33363101 http://dx.doi.org/10.3389/fchem.2020.546947 Text en Copyright © 2020 Wu, Zhou, Khenata, Kuang and Wang. http://creativecommons.org/licenses/by/4.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms. |
spellingShingle | Chemistry Wu, Mengxin Zhou, Feng Khenata, Rabah Kuang, Minquan Wang, Xiaotian Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni) |
title | Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni) |
title_full | Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni) |
title_fullStr | Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni) |
title_full_unstemmed | Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni) |
title_short | Phase Transition and Electronic Structures of All-d-Metal Heusler-Type X(2)MnTi Compounds (X = Pd, Pt, Ag, Au, Cu, and Ni) |
title_sort | phase transition and electronic structures of all-d-metal heusler-type x(2)mnti compounds (x = pd, pt, ag, au, cu, and ni) |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7759634/ https://www.ncbi.nlm.nih.gov/pubmed/33363101 http://dx.doi.org/10.3389/fchem.2020.546947 |
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