Superconductivity of cubic M B6 ( M = Na, K, Rb, Cs)
Previous studies have shown that NaB6, KB6, and RbB6 adopting Pm3̄m are superconductors with a relatively high Tc under ambient conditions. In this paper, we conducted systematic structural and related properties research on CsB6 through a genetic evolution algorithm and total energy calculations ba...
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creator | Chen, Shi Xie, Hui Xu, Dan Chen, Jiajin Cao, Bohan Liang, Min Sun, Yibo Gai, Xiaoqian Wang, Xinwei Yang, Mengxin Zhang, Mengrui Duan, Defang Li, Da Tian, Fubo |
description | Previous studies have shown that NaB6, KB6, and RbB6 adopting Pm3̄m are superconductors with a relatively high Tc under ambient conditions. In this paper, we conducted systematic structural and related properties research on CsB6 through a genetic evolution algorithm and total energy calculations based on density functional theory between 0 and 20 GPa. Our results reveal a cubic Pm3̄m CsB6, which is dynamically stable under the pressures we studied. We systematically calculated the formation enthalpies, electronic properties, and superconducting properties of Pm3̄m MB6 (M = Na, K, Rb, Cs). They all exhibit metallic features, and boron has high contributions to band structures, density of states, and electron–phonon coupling (EPC). The calculated results about the Helmholtz free energy difference of Pm3̄m CsB6 at 0, 10, and 20 GPa indicate that it is stable upon chemical decomposition (decomposition to simple substances Cs and B) from 0 to 400 K. The phonon density of states indicates that boron atoms occupy the high frequency area. The EPC results show that Pm3̄m CsB6 is a superconductor with Tc = 11.7 K at 0 GPa, close to NaB6 (13.1 K), KB6 (11.7 K), and RbB6 (11.3 K) at 0 GPa in our work, which indicates that boron atoms play an essential role in superconductivity: vibrations of B6 regular octagons lead to the high Tc of Pm3̄m MB6. Our work about Pm3̄m hexaborides provides a supplementary study on the borides of the group IA elements (without Fr and Li) and has an important guiding significance for the experimental synthesis of CsB6. |
doi_str_mv | 10.1063/5.0179339 |
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In this paper, we conducted systematic structural and related properties research on CsB6 through a genetic evolution algorithm and total energy calculations based on density functional theory between 0 and 20 GPa. Our results reveal a cubic Pm3̄m CsB6, which is dynamically stable under the pressures we studied. We systematically calculated the formation enthalpies, electronic properties, and superconducting properties of Pm3̄m MB6 (M = Na, K, Rb, Cs). They all exhibit metallic features, and boron has high contributions to band structures, density of states, and electron–phonon coupling (EPC). The calculated results about the Helmholtz free energy difference of Pm3̄m CsB6 at 0, 10, and 20 GPa indicate that it is stable upon chemical decomposition (decomposition to simple substances Cs and B) from 0 to 400 K. The phonon density of states indicates that boron atoms occupy the high frequency area. The EPC results show that Pm3̄m CsB6 is a superconductor with Tc = 11.7 K at 0 GPa, close to NaB6 (13.1 K), KB6 (11.7 K), and RbB6 (11.3 K) at 0 GPa in our work, which indicates that boron atoms play an essential role in superconductivity: vibrations of B6 regular octagons lead to the high Tc of Pm3̄m MB6. Our work about Pm3̄m hexaborides provides a supplementary study on the borides of the group IA elements (without Fr and Li) and has an important guiding significance for the experimental synthesis of CsB6.</description><identifier>ISSN: 0021-9606</identifier><identifier>EISSN: 1089-7690</identifier><identifier>DOI: 10.1063/5.0179339</identifier><language>eng</language><ispartof>The Journal of chemical physics, 2024-01, Vol.160 (4)</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c749-175b158ca225d087b03a5ddb7f915da6b43aafbc0a074373a421330002534713</citedby><cites>FETCH-LOGICAL-c749-175b158ca225d087b03a5ddb7f915da6b43aafbc0a074373a421330002534713</cites><orcidid>0009-0004-3897-0886 ; 0009-0001-2263-697X ; 0009-0003-9820-0333 ; 0009-0002-1052-3430 ; 0009-0002-9470-3438 ; 0000-0002-0041-9181 ; 0009-0001-4013-8202 ; 0000-0002-6878-1830 ; 0009-0000-6934-5910 ; 0000-0002-3490-2825 ; 0009-0006-1688-2281 ; 0000-0002-1147-4629 ; 0009-0003-9777-5426 ; 0000-0001-9352-4126</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Chen, Shi</creatorcontrib><creatorcontrib>Xie, Hui</creatorcontrib><creatorcontrib>Xu, Dan</creatorcontrib><creatorcontrib>Chen, Jiajin</creatorcontrib><creatorcontrib>Cao, Bohan</creatorcontrib><creatorcontrib>Liang, Min</creatorcontrib><creatorcontrib>Sun, Yibo</creatorcontrib><creatorcontrib>Gai, Xiaoqian</creatorcontrib><creatorcontrib>Wang, Xinwei</creatorcontrib><creatorcontrib>Yang, Mengxin</creatorcontrib><creatorcontrib>Zhang, Mengrui</creatorcontrib><creatorcontrib>Duan, Defang</creatorcontrib><creatorcontrib>Li, Da</creatorcontrib><creatorcontrib>Tian, Fubo</creatorcontrib><title>Superconductivity of cubic M B6 ( M = Na, K, Rb, Cs)</title><title>The Journal of chemical physics</title><description>Previous studies have shown that NaB6, KB6, and RbB6 adopting Pm3̄m are superconductors with a relatively high Tc under ambient conditions. In this paper, we conducted systematic structural and related properties research on CsB6 through a genetic evolution algorithm and total energy calculations based on density functional theory between 0 and 20 GPa. Our results reveal a cubic Pm3̄m CsB6, which is dynamically stable under the pressures we studied. We systematically calculated the formation enthalpies, electronic properties, and superconducting properties of Pm3̄m MB6 (M = Na, K, Rb, Cs). They all exhibit metallic features, and boron has high contributions to band structures, density of states, and electron–phonon coupling (EPC). The calculated results about the Helmholtz free energy difference of Pm3̄m CsB6 at 0, 10, and 20 GPa indicate that it is stable upon chemical decomposition (decomposition to simple substances Cs and B) from 0 to 400 K. The phonon density of states indicates that boron atoms occupy the high frequency area. The EPC results show that Pm3̄m CsB6 is a superconductor with Tc = 11.7 K at 0 GPa, close to NaB6 (13.1 K), KB6 (11.7 K), and RbB6 (11.3 K) at 0 GPa in our work, which indicates that boron atoms play an essential role in superconductivity: vibrations of B6 regular octagons lead to the high Tc of Pm3̄m MB6. Our work about Pm3̄m hexaborides provides a supplementary study on the borides of the group IA elements (without Fr and Li) and has an important guiding significance for the experimental synthesis of CsB6.</description><issn>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNotj81Kw0AURgdRMFYXvsEsLWTqvXPnJ7NwoUFtsSpY92FmkkBETck0Qt_eiF2dzcfHOYxdIiwQDF3rBaB1RO6IZQiFE9Y4OGYZgEThDJhTdpbSB8A0kypjajNumyH23_UYd91Pt9vzvuVxDF3kz_zO8KsJN_zF5_wp528h52Wan7OT1n-m5uLAGds83L-XS7F-fVyVt2sRrXICrQ6oi-il1DUUNgB5XdfBtg517U1Q5H0bIniwiix5JZFoMpOalEWasfn_axz6lIamrbZD9-WHfYVQ_cVWujrE0i_r-kFA</recordid><startdate>20240128</startdate><enddate>20240128</enddate><creator>Chen, Shi</creator><creator>Xie, Hui</creator><creator>Xu, Dan</creator><creator>Chen, Jiajin</creator><creator>Cao, Bohan</creator><creator>Liang, Min</creator><creator>Sun, Yibo</creator><creator>Gai, Xiaoqian</creator><creator>Wang, Xinwei</creator><creator>Yang, Mengxin</creator><creator>Zhang, Mengrui</creator><creator>Duan, Defang</creator><creator>Li, Da</creator><creator>Tian, Fubo</creator><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0009-0004-3897-0886</orcidid><orcidid>https://orcid.org/0009-0001-2263-697X</orcidid><orcidid>https://orcid.org/0009-0003-9820-0333</orcidid><orcidid>https://orcid.org/0009-0002-1052-3430</orcidid><orcidid>https://orcid.org/0009-0002-9470-3438</orcidid><orcidid>https://orcid.org/0000-0002-0041-9181</orcidid><orcidid>https://orcid.org/0009-0001-4013-8202</orcidid><orcidid>https://orcid.org/0000-0002-6878-1830</orcidid><orcidid>https://orcid.org/0009-0000-6934-5910</orcidid><orcidid>https://orcid.org/0000-0002-3490-2825</orcidid><orcidid>https://orcid.org/0009-0006-1688-2281</orcidid><orcidid>https://orcid.org/0000-0002-1147-4629</orcidid><orcidid>https://orcid.org/0009-0003-9777-5426</orcidid><orcidid>https://orcid.org/0000-0001-9352-4126</orcidid></search><sort><creationdate>20240128</creationdate><title>Superconductivity of cubic M B6 ( M = Na, K, Rb, Cs)</title><author>Chen, Shi ; Xie, Hui ; Xu, Dan ; Chen, Jiajin ; Cao, Bohan ; Liang, Min ; Sun, Yibo ; Gai, Xiaoqian ; Wang, Xinwei ; Yang, Mengxin ; Zhang, Mengrui ; Duan, Defang ; Li, Da ; Tian, Fubo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c749-175b158ca225d087b03a5ddb7f915da6b43aafbc0a074373a421330002534713</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chen, Shi</creatorcontrib><creatorcontrib>Xie, Hui</creatorcontrib><creatorcontrib>Xu, Dan</creatorcontrib><creatorcontrib>Chen, Jiajin</creatorcontrib><creatorcontrib>Cao, Bohan</creatorcontrib><creatorcontrib>Liang, Min</creatorcontrib><creatorcontrib>Sun, Yibo</creatorcontrib><creatorcontrib>Gai, Xiaoqian</creatorcontrib><creatorcontrib>Wang, Xinwei</creatorcontrib><creatorcontrib>Yang, Mengxin</creatorcontrib><creatorcontrib>Zhang, Mengrui</creatorcontrib><creatorcontrib>Duan, Defang</creatorcontrib><creatorcontrib>Li, Da</creatorcontrib><creatorcontrib>Tian, Fubo</creatorcontrib><collection>CrossRef</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chen, Shi</au><au>Xie, Hui</au><au>Xu, Dan</au><au>Chen, Jiajin</au><au>Cao, Bohan</au><au>Liang, Min</au><au>Sun, Yibo</au><au>Gai, Xiaoqian</au><au>Wang, Xinwei</au><au>Yang, Mengxin</au><au>Zhang, Mengrui</au><au>Duan, Defang</au><au>Li, Da</au><au>Tian, Fubo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Superconductivity of cubic M B6 ( M = Na, K, Rb, Cs)</atitle><jtitle>The Journal of chemical physics</jtitle><date>2024-01-28</date><risdate>2024</risdate><volume>160</volume><issue>4</issue><issn>0021-9606</issn><eissn>1089-7690</eissn><abstract>Previous studies have shown that NaB6, KB6, and RbB6 adopting Pm3̄m are superconductors with a relatively high Tc under ambient conditions. In this paper, we conducted systematic structural and related properties research on CsB6 through a genetic evolution algorithm and total energy calculations based on density functional theory between 0 and 20 GPa. Our results reveal a cubic Pm3̄m CsB6, which is dynamically stable under the pressures we studied. We systematically calculated the formation enthalpies, electronic properties, and superconducting properties of Pm3̄m MB6 (M = Na, K, Rb, Cs). They all exhibit metallic features, and boron has high contributions to band structures, density of states, and electron–phonon coupling (EPC). The calculated results about the Helmholtz free energy difference of Pm3̄m CsB6 at 0, 10, and 20 GPa indicate that it is stable upon chemical decomposition (decomposition to simple substances Cs and B) from 0 to 400 K. The phonon density of states indicates that boron atoms occupy the high frequency area. The EPC results show that Pm3̄m CsB6 is a superconductor with Tc = 11.7 K at 0 GPa, close to NaB6 (13.1 K), KB6 (11.7 K), and RbB6 (11.3 K) at 0 GPa in our work, which indicates that boron atoms play an essential role in superconductivity: vibrations of B6 regular octagons lead to the high Tc of Pm3̄m MB6. 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title | Superconductivity of cubic M B6 ( M = Na, K, Rb, Cs) |
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