Modified transverse Ising model for the dielectric properties of SrTiO 3 films and interfaces
The transverse Ising model (TIM), with pseudospins representing the lattice polarization, is often used as a simple description of ferroelectric materials. However, we demonstrate that the TIM, as it is usually formulated, provides an incorrect description of SrTiO films and interfaces because of it...
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Veröffentlicht in: | Journal of physics. Condensed matter 2020-02, Vol.32 (6), p.065303 |
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creator | Chapman, Kelsey S Atkinson, W A |
description | The transverse Ising model (TIM), with pseudospins representing the lattice polarization, is often used as a simple description of ferroelectric materials. However, we demonstrate that the TIM, as it is usually formulated, provides an incorrect description of SrTiO
films and interfaces because of its inadequate treatment of spatial inhomogeneity. We correct this deficiency by adding a pseudospin anisotropy to the model. We demonstrate the physical need for this term by comparison of the TIM to a typical Landau-Ginzburg-Devonshire model. We then demonstrate the physical consequences of the modification for two model systems: a ferroelectric thin film, and a metallic LaAlO
/SrTiO
interface. We show that, in both cases, the modified TIM has a substantially different polarization profile than the conventional TIM. In particular, at low temperatures the formation of quantized states at LaAlO
/SrTiO
interfaces only occurs in the modified TIM. |
doi_str_mv | 10.1088/1361-648X/ab4fa7 |
format | Article |
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films and interfaces because of its inadequate treatment of spatial inhomogeneity. We correct this deficiency by adding a pseudospin anisotropy to the model. We demonstrate the physical need for this term by comparison of the TIM to a typical Landau-Ginzburg-Devonshire model. We then demonstrate the physical consequences of the modification for two model systems: a ferroelectric thin film, and a metallic LaAlO
/SrTiO
interface. We show that, in both cases, the modified TIM has a substantially different polarization profile than the conventional TIM. In particular, at low temperatures the formation of quantized states at LaAlO
/SrTiO
interfaces only occurs in the modified TIM.</description><identifier>ISSN: 0953-8984</identifier><identifier>EISSN: 1361-648X</identifier><identifier>DOI: 10.1088/1361-648X/ab4fa7</identifier><identifier>PMID: 31634883</identifier><language>eng</language><publisher>England</publisher><ispartof>Journal of physics. Condensed matter, 2020-02, Vol.32 (6), p.065303</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1113-2714ed596f369f526ee6f4994d166dbce60f55233c748c96b89258dc92f4acad3</citedby><cites>FETCH-LOGICAL-c1113-2714ed596f369f526ee6f4994d166dbce60f55233c748c96b89258dc92f4acad3</cites><orcidid>0000-0002-3427-219X ; 0000-0002-9279-1748</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/31634883$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Chapman, Kelsey S</creatorcontrib><creatorcontrib>Atkinson, W A</creatorcontrib><title>Modified transverse Ising model for the dielectric properties of SrTiO 3 films and interfaces</title><title>Journal of physics. Condensed matter</title><addtitle>J Phys Condens Matter</addtitle><description>The transverse Ising model (TIM), with pseudospins representing the lattice polarization, is often used as a simple description of ferroelectric materials. However, we demonstrate that the TIM, as it is usually formulated, provides an incorrect description of SrTiO
films and interfaces because of its inadequate treatment of spatial inhomogeneity. We correct this deficiency by adding a pseudospin anisotropy to the model. We demonstrate the physical need for this term by comparison of the TIM to a typical Landau-Ginzburg-Devonshire model. We then demonstrate the physical consequences of the modification for two model systems: a ferroelectric thin film, and a metallic LaAlO
/SrTiO
interface. We show that, in both cases, the modified TIM has a substantially different polarization profile than the conventional TIM. In particular, at low temperatures the formation of quantized states at LaAlO
/SrTiO
interfaces only occurs in the modified TIM.</description><issn>0953-8984</issn><issn>1361-648X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNo90EtLAzEUhuEgih2re1eSPzA2mZNJk6UUL4VKF1ZwI0MmOdHI3EhGwX-vQ7WrAwfeb_EQcsnZNWdKLThInkuhXhamFt4sj0h2eB2TjOkScqWVmJGzlD4YY0KBOCUz4BKEUpCR18feBR_Q0TGaLn1hTEjXKXRvtO0dNtT3kY7vSF3ABu0Yg6VD7AeMY8BEe0-f4i5sKVAfmjZR0zkauhGjNxbTOTnxpkl48Xfn5Pnudrd6yDfb-_XqZpNbzjnkxZILdKWWHqT2ZSERpRdaC8eldLVFyXxZFgB2KZTVsla6KJWzuvDCWONgTth-18Y-pYi-GmJoTfyuOKsmqWpiqSaWai_1m1ztk-GzbtEdgn8a-AFrU2Wh</recordid><startdate>20200206</startdate><enddate>20200206</enddate><creator>Chapman, Kelsey S</creator><creator>Atkinson, W A</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-3427-219X</orcidid><orcidid>https://orcid.org/0000-0002-9279-1748</orcidid></search><sort><creationdate>20200206</creationdate><title>Modified transverse Ising model for the dielectric properties of SrTiO 3 films and interfaces</title><author>Chapman, Kelsey S ; Atkinson, W A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1113-2714ed596f369f526ee6f4994d166dbce60f55233c748c96b89258dc92f4acad3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chapman, Kelsey S</creatorcontrib><creatorcontrib>Atkinson, W A</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><jtitle>Journal of physics. Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chapman, Kelsey S</au><au>Atkinson, W A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Modified transverse Ising model for the dielectric properties of SrTiO 3 films and interfaces</atitle><jtitle>Journal of physics. Condensed matter</jtitle><addtitle>J Phys Condens Matter</addtitle><date>2020-02-06</date><risdate>2020</risdate><volume>32</volume><issue>6</issue><spage>065303</spage><pages>065303-</pages><issn>0953-8984</issn><eissn>1361-648X</eissn><abstract>The transverse Ising model (TIM), with pseudospins representing the lattice polarization, is often used as a simple description of ferroelectric materials. However, we demonstrate that the TIM, as it is usually formulated, provides an incorrect description of SrTiO
films and interfaces because of its inadequate treatment of spatial inhomogeneity. We correct this deficiency by adding a pseudospin anisotropy to the model. We demonstrate the physical need for this term by comparison of the TIM to a typical Landau-Ginzburg-Devonshire model. We then demonstrate the physical consequences of the modification for two model systems: a ferroelectric thin film, and a metallic LaAlO
/SrTiO
interface. We show that, in both cases, the modified TIM has a substantially different polarization profile than the conventional TIM. In particular, at low temperatures the formation of quantized states at LaAlO
/SrTiO
interfaces only occurs in the modified TIM.</abstract><cop>England</cop><pmid>31634883</pmid><doi>10.1088/1361-648X/ab4fa7</doi><orcidid>https://orcid.org/0000-0002-3427-219X</orcidid><orcidid>https://orcid.org/0000-0002-9279-1748</orcidid></addata></record> |
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title | Modified transverse Ising model for the dielectric properties of SrTiO 3 films and interfaces |
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