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Superconducting Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg Theory
[Image: see text] Motivated by Matthias’ sixth rule for finding new superconducting materials in a cubic symmetry, we report the cluster expansion calculations, based on the density functional theory, of the superconducting properties of Al(0.5)Zr(0.5)H(3). The Al(0.5)Zr(0.5)H(3) structure is thermo...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2022
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9386819/ https://www.ncbi.nlm.nih.gov/pubmed/35990471 http://dx.doi.org/10.1021/acsomega.2c02447 |
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author | Tsuppayakorn-aek, Prutthipong Ahuja, Rajeev Bovornratanaraks, Thiti Luo, Wei |
author_facet | Tsuppayakorn-aek, Prutthipong Ahuja, Rajeev Bovornratanaraks, Thiti Luo, Wei |
author_sort | Tsuppayakorn-aek, Prutthipong |
collection | PubMed |
description | [Image: see text] Motivated by Matthias’ sixth rule for finding new superconducting materials in a cubic symmetry, we report the cluster expansion calculations, based on the density functional theory, of the superconducting properties of Al(0.5)Zr(0.5)H(3). The Al(0.5)Zr(0.5)H(3) structure is thermodynamically and dynamically stable up to at least 200 GPa. The structural properties suggest that the Al(0.5)Zr(0.5)H(3) structure is a metallic. We calculate a superconducting transition temperature using the Allen–Dynes modified McMillan equation and anisotropic Migdal–Eliashberg equation. As result of this, the anisotropic Migdal–Eliashberg equation demonstrated that it exhibits superconductivity under high pressure with relatively high-T(c) of 55.3 K at a pressure of 100 GPa among a family of simple cubic structures. Therefore, these findings suggest that superconductivity could be observed experimentally in Al(0.5)Zr(0.5)H(3). |
format | Online Article Text |
id | pubmed-9386819 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-93868192022-08-19 Superconducting Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg Theory Tsuppayakorn-aek, Prutthipong Ahuja, Rajeev Bovornratanaraks, Thiti Luo, Wei ACS Omega [Image: see text] Motivated by Matthias’ sixth rule for finding new superconducting materials in a cubic symmetry, we report the cluster expansion calculations, based on the density functional theory, of the superconducting properties of Al(0.5)Zr(0.5)H(3). The Al(0.5)Zr(0.5)H(3) structure is thermodynamically and dynamically stable up to at least 200 GPa. The structural properties suggest that the Al(0.5)Zr(0.5)H(3) structure is a metallic. We calculate a superconducting transition temperature using the Allen–Dynes modified McMillan equation and anisotropic Migdal–Eliashberg equation. As result of this, the anisotropic Migdal–Eliashberg equation demonstrated that it exhibits superconductivity under high pressure with relatively high-T(c) of 55.3 K at a pressure of 100 GPa among a family of simple cubic structures. Therefore, these findings suggest that superconductivity could be observed experimentally in Al(0.5)Zr(0.5)H(3). American Chemical Society 2022-08-01 /pmc/articles/PMC9386819/ /pubmed/35990471 http://dx.doi.org/10.1021/acsomega.2c02447 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/). |
spellingShingle | Tsuppayakorn-aek, Prutthipong Ahuja, Rajeev Bovornratanaraks, Thiti Luo, Wei Superconducting Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg Theory |
title | Superconducting
Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg
Theory |
title_full | Superconducting
Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg
Theory |
title_fullStr | Superconducting
Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg
Theory |
title_full_unstemmed | Superconducting
Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg
Theory |
title_short | Superconducting
Gap of Pressure Stabilized (Al(0.5)Zr(0.5))H(3) from Ab Initio Anisotropic Migdal–Eliashberg
Theory |
title_sort | superconducting
gap of pressure stabilized (al(0.5)zr(0.5))h(3) from ab initio anisotropic migdal–eliashberg
theory |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9386819/ https://www.ncbi.nlm.nih.gov/pubmed/35990471 http://dx.doi.org/10.1021/acsomega.2c02447 |
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