Metal-Insulator Transition of c-Axis-Controlled V sub( 2)O sub( 3) Thin Film
We prepared c-axis-controlled V sub(2)O sub(3) thin films by RF magnetron sputtering and proved their metal-insulator transition (MIT) in terms of electronic structure. The lattice constant of the c-axis depends on the film thickness and the lattice mismatch of the substrate and V sub(2)O sub(3). MI...
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Veröffentlicht in: | Journal of the Physical Society of Japan 2015-06, Vol.84 (6), p.1-1 |
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container_title | Journal of the Physical Society of Japan |
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creator | Shimazu, Yuichi Okumura, Teppei Tsuchiya, Takashi Shimada, Atsushi Tanabe, Kenji Tokiwa, Kazuyasu Kobayashi, Masaki Horiba, Koji Kumigashira, Hiroshi Higuchi, Tohru |
description | We prepared c-axis-controlled V sub(2)O sub(3) thin films by RF magnetron sputtering and proved their metal-insulator transition (MIT) in terms of electronic structure. The lattice constant of the c-axis depends on the film thickness and the lattice mismatch of the substrate and V sub(2)O sub(3). MIT is observed at a temperature of ~150 K in the V sub(2)O sub(3) thin films with the lattice constants of c = 13.942 and 13.992 A, although the V sub(2)O sub(3) thin film with c = 13.915 A exhibits metallic conductivity without MIT. The electron correlation energy, which corresponds to the energy difference between the lower Hubbard band and the upper Hubbard band, increases with increasing lattice constant of the c-axis. Bandwidths also depend on the lattice constant of the c-axis. The intensity of the a1g orbital around the Fermi level decreases with increasing lattice constant of the c-axis. These results suggest that the electron correlation interaction and bandwidths play important roles in the MIT of c-axis-controlled V sub(2)O sub(3) thin films. |
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The lattice constant of the c-axis depends on the film thickness and the lattice mismatch of the substrate and V sub(2)O sub(3). MIT is observed at a temperature of ~150 K in the V sub(2)O sub(3) thin films with the lattice constants of c = 13.942 and 13.992 A, although the V sub(2)O sub(3) thin film with c = 13.915 A exhibits metallic conductivity without MIT. The electron correlation energy, which corresponds to the energy difference between the lower Hubbard band and the upper Hubbard band, increases with increasing lattice constant of the c-axis. Bandwidths also depend on the lattice constant of the c-axis. The intensity of the a1g orbital around the Fermi level decreases with increasing lattice constant of the c-axis. These results suggest that the electron correlation interaction and bandwidths play important roles in the MIT of c-axis-controlled V sub(2)O sub(3) thin films.</description><identifier>ISSN: 0031-9015</identifier><identifier>EISSN: 1347-4073</identifier><language>eng</language><subject>Correlation ; Electronic structure ; Film thickness ; Lattice parameters ; Lattices ; Metal-insulator transition ; Symbols ; Thin films</subject><ispartof>Journal of the Physical Society of Japan, 2015-06, Vol.84 (6), p.1-1</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780</link.rule.ids></links><search><creatorcontrib>Shimazu, Yuichi</creatorcontrib><creatorcontrib>Okumura, Teppei</creatorcontrib><creatorcontrib>Tsuchiya, Takashi</creatorcontrib><creatorcontrib>Shimada, Atsushi</creatorcontrib><creatorcontrib>Tanabe, Kenji</creatorcontrib><creatorcontrib>Tokiwa, Kazuyasu</creatorcontrib><creatorcontrib>Kobayashi, Masaki</creatorcontrib><creatorcontrib>Horiba, Koji</creatorcontrib><creatorcontrib>Kumigashira, Hiroshi</creatorcontrib><creatorcontrib>Higuchi, Tohru</creatorcontrib><title>Metal-Insulator Transition of c-Axis-Controlled V sub( 2)O sub( 3) Thin Film</title><title>Journal of the Physical Society of Japan</title><description>We prepared c-axis-controlled V sub(2)O sub(3) thin films by RF magnetron sputtering and proved their metal-insulator transition (MIT) in terms of electronic structure. The lattice constant of the c-axis depends on the film thickness and the lattice mismatch of the substrate and V sub(2)O sub(3). MIT is observed at a temperature of ~150 K in the V sub(2)O sub(3) thin films with the lattice constants of c = 13.942 and 13.992 A, although the V sub(2)O sub(3) thin film with c = 13.915 A exhibits metallic conductivity without MIT. The electron correlation energy, which corresponds to the energy difference between the lower Hubbard band and the upper Hubbard band, increases with increasing lattice constant of the c-axis. Bandwidths also depend on the lattice constant of the c-axis. The intensity of the a1g orbital around the Fermi level decreases with increasing lattice constant of the c-axis. These results suggest that the electron correlation interaction and bandwidths play important roles in the MIT of c-axis-controlled V sub(2)O sub(3) thin films.</description><subject>Correlation</subject><subject>Electronic structure</subject><subject>Film thickness</subject><subject>Lattice parameters</subject><subject>Lattices</subject><subject>Metal-insulator transition</subject><subject>Symbols</subject><subject>Thin films</subject><issn>0031-9015</issn><issn>1347-4073</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqFjstKAzEARYMoOFb_Ict2Ecj7sSzFamGkm8FtyeSBkTSpkxnw8xXq3tU9i8Ph3oCOMK4Qx4rdgg5jRpDBRNyDh9Y-MaaCUN6B_i3MNqNDaUu2c53gMNnS0pxqgTVCh7bfqaFdLfNUcw4evsO2jGtIN8crsA0cPlKB-5TPj-Au2tzC09-uwLB_HnavqD--HHbbHl2kZIhLzqPEXnritHeUEG-5HKkWXnsWvfLWRKkjs466wCVRo3dG8qB-_0vj2Qqsr9nLVL-W0ObTOTUXcrYl1KWdiKbMcKEZ-19V2CgpCBbsBy9hV9Q</recordid><startdate>20150601</startdate><enddate>20150601</enddate><creator>Shimazu, Yuichi</creator><creator>Okumura, Teppei</creator><creator>Tsuchiya, Takashi</creator><creator>Shimada, Atsushi</creator><creator>Tanabe, Kenji</creator><creator>Tokiwa, Kazuyasu</creator><creator>Kobayashi, Masaki</creator><creator>Horiba, Koji</creator><creator>Kumigashira, Hiroshi</creator><creator>Higuchi, Tohru</creator><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7U7</scope><scope>C1K</scope></search><sort><creationdate>20150601</creationdate><title>Metal-Insulator Transition of c-Axis-Controlled V sub( 2)O sub( 3) Thin Film</title><author>Shimazu, Yuichi ; Okumura, Teppei ; Tsuchiya, Takashi ; Shimada, Atsushi ; Tanabe, Kenji ; Tokiwa, Kazuyasu ; Kobayashi, Masaki ; Horiba, Koji ; Kumigashira, Hiroshi ; Higuchi, Tohru</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p663-4644f60d6d1c8dc211da46b285d8d3fd7da9f68f3ac2ce4617bdc964e790169d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Correlation</topic><topic>Electronic structure</topic><topic>Film thickness</topic><topic>Lattice parameters</topic><topic>Lattices</topic><topic>Metal-insulator transition</topic><topic>Symbols</topic><topic>Thin films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shimazu, Yuichi</creatorcontrib><creatorcontrib>Okumura, Teppei</creatorcontrib><creatorcontrib>Tsuchiya, Takashi</creatorcontrib><creatorcontrib>Shimada, Atsushi</creatorcontrib><creatorcontrib>Tanabe, Kenji</creatorcontrib><creatorcontrib>Tokiwa, Kazuyasu</creatorcontrib><creatorcontrib>Kobayashi, Masaki</creatorcontrib><creatorcontrib>Horiba, Koji</creatorcontrib><creatorcontrib>Kumigashira, Hiroshi</creatorcontrib><creatorcontrib>Higuchi, Tohru</creatorcontrib><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Toxicology Abstracts</collection><collection>Environmental Sciences and Pollution Management</collection><jtitle>Journal of the Physical Society of Japan</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shimazu, Yuichi</au><au>Okumura, Teppei</au><au>Tsuchiya, Takashi</au><au>Shimada, Atsushi</au><au>Tanabe, Kenji</au><au>Tokiwa, Kazuyasu</au><au>Kobayashi, Masaki</au><au>Horiba, Koji</au><au>Kumigashira, Hiroshi</au><au>Higuchi, Tohru</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Metal-Insulator Transition of c-Axis-Controlled V sub( 2)O sub( 3) Thin Film</atitle><jtitle>Journal of the Physical Society of Japan</jtitle><date>2015-06-01</date><risdate>2015</risdate><volume>84</volume><issue>6</issue><spage>1</spage><epage>1</epage><pages>1-1</pages><issn>0031-9015</issn><eissn>1347-4073</eissn><abstract>We prepared c-axis-controlled V sub(2)O sub(3) thin films by RF magnetron sputtering and proved their metal-insulator transition (MIT) in terms of electronic structure. The lattice constant of the c-axis depends on the film thickness and the lattice mismatch of the substrate and V sub(2)O sub(3). MIT is observed at a temperature of ~150 K in the V sub(2)O sub(3) thin films with the lattice constants of c = 13.942 and 13.992 A, although the V sub(2)O sub(3) thin film with c = 13.915 A exhibits metallic conductivity without MIT. The electron correlation energy, which corresponds to the energy difference between the lower Hubbard band and the upper Hubbard band, increases with increasing lattice constant of the c-axis. Bandwidths also depend on the lattice constant of the c-axis. The intensity of the a1g orbital around the Fermi level decreases with increasing lattice constant of the c-axis. These results suggest that the electron correlation interaction and bandwidths play important roles in the MIT of c-axis-controlled V sub(2)O sub(3) thin films.</abstract><tpages>1</tpages></addata></record> |
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subjects | Correlation Electronic structure Film thickness Lattice parameters Lattices Metal-insulator transition Symbols Thin films |
title | Metal-Insulator Transition of c-Axis-Controlled V sub( 2)O sub( 3) Thin Film |
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