Predicting the structural, electronic and magnetic properties of few atomic-layer polar perovskite
Density functional theory (DFT) calculations are performed to predict the structural, electronic and magnetic properties of electrically neutral or charged few-atomic-layer (AL) oxides based on polar perovskite KTaO 3 . Their properties vary greatly with the number of ALs ( n AL ) and the stoichiome...
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Veröffentlicht in: | Physical chemistry chemical physics : PCCP 2021-03, Vol.23 (9), p.5578-5582 |
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creator | Xu, Shaowen Jia, Fanhao Hu, Shunbo Sundaresan, Athinarayanan Ter-Oganessian, Nikita V Pyatakov, Alexander P Cheng, Jinrong Zhang, Jincang Cao, Shixun Ren§, Wei |
description | Density functional theory (DFT) calculations are performed to predict the structural, electronic and magnetic properties of electrically neutral or charged few-atomic-layer (AL) oxides based on polar perovskite KTaO
3
. Their properties vary greatly with the number of ALs (
n
AL
) and the stoichiometric ratio. In the few-AL limit (
n
AL
≤ 14), the even AL (EL) systems with the chemical formula (KTaO
3
)
n
are semiconductors, while the odd AL (OL) systems with the formula K
n
+1
Ta
n
O
3
n
+1
or K
n
Ta
n
+1
O
3
n
+2
are half-metal except for the unique KTa
2
O
5
case which is a semiconductor due to the large Peierls distortions. After reaching a certain critical thickness (
n
AL
> 14), the EL systems show ferromagnetic surface states, while ferromagnetism disappears in the OL systems. These predictions from fundamental complexity of polar perovskite when approaching the two-dimensional (2D) limit may be helpful for interpreting experimental observations later.
Density functional theory predictions of polar perovskite KTaO
3
when approaching the two-dimensional (2D) limit for electrically neutral and charged few-atomic-layer cases. |
doi_str_mv | 10.1039/d0cp06671k |
format | Article |
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3
. Their properties vary greatly with the number of ALs (
n
AL
) and the stoichiometric ratio. In the few-AL limit (
n
AL
≤ 14), the even AL (EL) systems with the chemical formula (KTaO
3
)
n
are semiconductors, while the odd AL (OL) systems with the formula K
n
+1
Ta
n
O
3
n
+1
or K
n
Ta
n
+1
O
3
n
+2
are half-metal except for the unique KTa
2
O
5
case which is a semiconductor due to the large Peierls distortions. After reaching a certain critical thickness (
n
AL
> 14), the EL systems show ferromagnetic surface states, while ferromagnetism disappears in the OL systems. These predictions from fundamental complexity of polar perovskite when approaching the two-dimensional (2D) limit may be helpful for interpreting experimental observations later.
Density functional theory predictions of polar perovskite KTaO
3
when approaching the two-dimensional (2D) limit for electrically neutral and charged few-atomic-layer cases.</description><identifier>ISSN: 1463-9076</identifier><identifier>EISSN: 1463-9084</identifier><identifier>DOI: 10.1039/d0cp06671k</identifier><identifier>PMID: 33655285</identifier><language>eng</language><publisher>England: Royal Society of Chemistry</publisher><subject>Density functional theory ; Ferromagnetism ; Magnetic properties ; Perovskites</subject><ispartof>Physical chemistry chemical physics : PCCP, 2021-03, Vol.23 (9), p.5578-5582</ispartof><rights>Copyright Royal Society of Chemistry 2021</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c374t-85867a697798db645cd2aefccb6505731762924723545454cf62e9d673702b613</citedby><cites>FETCH-LOGICAL-c374t-85867a697798db645cd2aefccb6505731762924723545454cf62e9d673702b613</cites><orcidid>0000-0002-9645-8395 ; 0000-0001-8965-1800 ; 0000-0001-7773-1133 ; 0000-0001-7317-3867 ; 0000-0002-1613-3030 ; 0000-0002-3915-2621</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,27905,27906</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/33655285$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Xu, Shaowen</creatorcontrib><creatorcontrib>Jia, Fanhao</creatorcontrib><creatorcontrib>Hu, Shunbo</creatorcontrib><creatorcontrib>Sundaresan, Athinarayanan</creatorcontrib><creatorcontrib>Ter-Oganessian, Nikita V</creatorcontrib><creatorcontrib>Pyatakov, Alexander P</creatorcontrib><creatorcontrib>Cheng, Jinrong</creatorcontrib><creatorcontrib>Zhang, Jincang</creatorcontrib><creatorcontrib>Cao, Shixun</creatorcontrib><creatorcontrib>Ren§, Wei</creatorcontrib><title>Predicting the structural, electronic and magnetic properties of few atomic-layer polar perovskite</title><title>Physical chemistry chemical physics : PCCP</title><addtitle>Phys Chem Chem Phys</addtitle><description>Density functional theory (DFT) calculations are performed to predict the structural, electronic and magnetic properties of electrically neutral or charged few-atomic-layer (AL) oxides based on polar perovskite KTaO
3
. Their properties vary greatly with the number of ALs (
n
AL
) and the stoichiometric ratio. In the few-AL limit (
n
AL
≤ 14), the even AL (EL) systems with the chemical formula (KTaO
3
)
n
are semiconductors, while the odd AL (OL) systems with the formula K
n
+1
Ta
n
O
3
n
+1
or K
n
Ta
n
+1
O
3
n
+2
are half-metal except for the unique KTa
2
O
5
case which is a semiconductor due to the large Peierls distortions. After reaching a certain critical thickness (
n
AL
> 14), the EL systems show ferromagnetic surface states, while ferromagnetism disappears in the OL systems. These predictions from fundamental complexity of polar perovskite when approaching the two-dimensional (2D) limit may be helpful for interpreting experimental observations later.
Density functional theory predictions of polar perovskite KTaO
3
when approaching the two-dimensional (2D) limit for electrically neutral and charged few-atomic-layer cases.</description><subject>Density functional theory</subject><subject>Ferromagnetism</subject><subject>Magnetic properties</subject><subject>Perovskites</subject><issn>1463-9076</issn><issn>1463-9084</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNpd0UtLxDAQB_Agiu-LdyXgRcRqHk3SHGV9ouAe9FzSdKrVtqlJqvjt7brrChJIJuTHMPyD0B4lp5RwfVYS2xMpFX1bQZs0lTzRJEtXl7WSG2grhFdCCBWUr6MNzqUQLBObqJh6KGsb6-4ZxxfAIfrBxsGb5gRDAzZ619UWm67ErXnuII6X3rsefKwhYFfhCj6xia6tbdKYL_C4d40Zd_DuI7zVEXbQWmWaALuLcxs9XV0-Tm6S-4fr28n5fWK5SmOSiUwqI7VSOisLmQpbMgOVtYUURChOlWSapYpxkc6WrSQDXUrFFWGFpHwbHc37jvO9DxBi3tbBQtOYDtwQcpZqyVJGiR7p4T_66gbfjdPNlM5oxiQZ1fFcWe9C8FDlva9b479ySvJZ8vkFmUx_kr8b8cGi5VC0UC7pb9Qj2J8DH-zy9e_r-Dd6VYdI</recordid><startdate>20210311</startdate><enddate>20210311</enddate><creator>Xu, Shaowen</creator><creator>Jia, Fanhao</creator><creator>Hu, Shunbo</creator><creator>Sundaresan, Athinarayanan</creator><creator>Ter-Oganessian, Nikita V</creator><creator>Pyatakov, Alexander P</creator><creator>Cheng, Jinrong</creator><creator>Zhang, Jincang</creator><creator>Cao, Shixun</creator><creator>Ren§, Wei</creator><general>Royal Society of Chemistry</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0002-9645-8395</orcidid><orcidid>https://orcid.org/0000-0001-8965-1800</orcidid><orcidid>https://orcid.org/0000-0001-7773-1133</orcidid><orcidid>https://orcid.org/0000-0001-7317-3867</orcidid><orcidid>https://orcid.org/0000-0002-1613-3030</orcidid><orcidid>https://orcid.org/0000-0002-3915-2621</orcidid></search><sort><creationdate>20210311</creationdate><title>Predicting the structural, electronic and magnetic properties of few atomic-layer polar perovskite</title><author>Xu, Shaowen ; Jia, Fanhao ; Hu, Shunbo ; Sundaresan, Athinarayanan ; Ter-Oganessian, Nikita V ; Pyatakov, Alexander P ; Cheng, Jinrong ; Zhang, Jincang ; Cao, Shixun ; Ren§, Wei</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c374t-85867a697798db645cd2aefccb6505731762924723545454cf62e9d673702b613</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Density functional theory</topic><topic>Ferromagnetism</topic><topic>Magnetic properties</topic><topic>Perovskites</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Xu, Shaowen</creatorcontrib><creatorcontrib>Jia, Fanhao</creatorcontrib><creatorcontrib>Hu, Shunbo</creatorcontrib><creatorcontrib>Sundaresan, Athinarayanan</creatorcontrib><creatorcontrib>Ter-Oganessian, Nikita V</creatorcontrib><creatorcontrib>Pyatakov, Alexander P</creatorcontrib><creatorcontrib>Cheng, Jinrong</creatorcontrib><creatorcontrib>Zhang, Jincang</creatorcontrib><creatorcontrib>Cao, Shixun</creatorcontrib><creatorcontrib>Ren§, Wei</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Physical chemistry chemical physics : PCCP</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Xu, Shaowen</au><au>Jia, Fanhao</au><au>Hu, Shunbo</au><au>Sundaresan, Athinarayanan</au><au>Ter-Oganessian, Nikita V</au><au>Pyatakov, Alexander P</au><au>Cheng, Jinrong</au><au>Zhang, Jincang</au><au>Cao, Shixun</au><au>Ren§, Wei</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Predicting the structural, electronic and magnetic properties of few atomic-layer polar perovskite</atitle><jtitle>Physical chemistry chemical physics : PCCP</jtitle><addtitle>Phys Chem Chem Phys</addtitle><date>2021-03-11</date><risdate>2021</risdate><volume>23</volume><issue>9</issue><spage>5578</spage><epage>5582</epage><pages>5578-5582</pages><issn>1463-9076</issn><eissn>1463-9084</eissn><abstract>Density functional theory (DFT) calculations are performed to predict the structural, electronic and magnetic properties of electrically neutral or charged few-atomic-layer (AL) oxides based on polar perovskite KTaO
3
. Their properties vary greatly with the number of ALs (
n
AL
) and the stoichiometric ratio. In the few-AL limit (
n
AL
≤ 14), the even AL (EL) systems with the chemical formula (KTaO
3
)
n
are semiconductors, while the odd AL (OL) systems with the formula K
n
+1
Ta
n
O
3
n
+1
or K
n
Ta
n
+1
O
3
n
+2
are half-metal except for the unique KTa
2
O
5
case which is a semiconductor due to the large Peierls distortions. After reaching a certain critical thickness (
n
AL
> 14), the EL systems show ferromagnetic surface states, while ferromagnetism disappears in the OL systems. These predictions from fundamental complexity of polar perovskite when approaching the two-dimensional (2D) limit may be helpful for interpreting experimental observations later.
Density functional theory predictions of polar perovskite KTaO
3
when approaching the two-dimensional (2D) limit for electrically neutral and charged few-atomic-layer cases.</abstract><cop>England</cop><pub>Royal Society of Chemistry</pub><pmid>33655285</pmid><doi>10.1039/d0cp06671k</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0002-9645-8395</orcidid><orcidid>https://orcid.org/0000-0001-8965-1800</orcidid><orcidid>https://orcid.org/0000-0001-7773-1133</orcidid><orcidid>https://orcid.org/0000-0001-7317-3867</orcidid><orcidid>https://orcid.org/0000-0002-1613-3030</orcidid><orcidid>https://orcid.org/0000-0002-3915-2621</orcidid></addata></record> |
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language | eng |
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source | Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
subjects | Density functional theory Ferromagnetism Magnetic properties Perovskites |
title | Predicting the structural, electronic and magnetic properties of few atomic-layer polar perovskite |
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