Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu sub(2) O
The negative thermal expansion (NTE) mechanism in Cu sub(2) O has been characterized via mapping of different Cu sub(2) O structural flexibility models onto phonons obtained using ab initio lattice dynamics. Low-frequency acoustic modes that are responsible for the NTE in this material correspond to...
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Veröffentlicht in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2014-06, Vol.89 (21) |
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creator | Rimmer, Leila H N Dove, Martin T Winkler, Bjorn Wilson, Dan J Refson, Keith Goodwin, Andrew L |
description | The negative thermal expansion (NTE) mechanism in Cu sub(2) O has been characterized via mapping of different Cu sub(2) O structural flexibility models onto phonons obtained using ab initio lattice dynamics. Low-frequency acoustic modes that are responsible for the NTE in this material correspond to vibrations of rigid O-Cu-O rods. There is also some small contribution from higher-frequency optic modes that correspond to rotations of rigid and near-rigid OCu sub(4) tetrahedra as well as of near-rigid O-Cu-O rods. The primary NTE mode also drives a ferroelastic phase transition at high pressure; our calculations predict this to be an orthorhombic structure with space group Pnnn. |
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Low-frequency acoustic modes that are responsible for the NTE in this material correspond to vibrations of rigid O-Cu-O rods. There is also some small contribution from higher-frequency optic modes that correspond to rotations of rigid and near-rigid OCu sub(4) tetrahedra as well as of near-rigid O-Cu-O rods. The primary NTE mode also drives a ferroelastic phase transition at high pressure; our calculations predict this to be an orthorhombic structure with space group Pnnn.</description><identifier>ISSN: 1098-0121</identifier><identifier>EISSN: 1550-235X</identifier><language>eng</language><subject>Condensed matter ; Dynamics ; Flexibility ; Lattice vibration ; Lattices ; LATTICES (CRYSTAL) ; OXIDES ; Rods ; Thermal expansion ; THERMAL EXPANSION COEFFICIENT ; Vibration</subject><ispartof>Physical review. 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The primary NTE mode also drives a ferroelastic phase transition at high pressure; our calculations predict this to be an orthorhombic structure with space group Pnnn.</description><subject>Condensed matter</subject><subject>Dynamics</subject><subject>Flexibility</subject><subject>Lattice vibration</subject><subject>Lattices</subject><subject>LATTICES (CRYSTAL)</subject><subject>OXIDES</subject><subject>Rods</subject><subject>Thermal expansion</subject><subject>THERMAL EXPANSION COEFFICIENT</subject><subject>Vibration</subject><issn>1098-0121</issn><issn>1550-235X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNqViruOwjAQAC0EEs9_2DIUkWyHCKgRCCoaiuvQEjZg8CN4Ewh_f4fED1w1M9J0xEDluUx1lv90_1wuF6lUWvXFkPkmpZotZ3ogcBPR0SvEO5SWWnMy1tRvQH-G-krg6YK1edInokML1Fbo2QQPjooresMOQglFqCqKyW4KoTVnglUD3JwSPYX9WPRKtEyTL0ci2awPq21axfBoiOujM1yQtegpNHxUc6lkli2Uzv6x_gImV0md</recordid><startdate>20140601</startdate><enddate>20140601</enddate><creator>Rimmer, Leila H N</creator><creator>Dove, Martin T</creator><creator>Winkler, Bjorn</creator><creator>Wilson, Dan J</creator><creator>Refson, Keith</creator><creator>Goodwin, Andrew L</creator><scope>7SR</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>H8G</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20140601</creationdate><title>Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu sub(2) O</title><author>Rimmer, Leila H N ; Dove, Martin T ; Winkler, Bjorn ; Wilson, Dan J ; Refson, Keith ; Goodwin, Andrew L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_17010338123</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Condensed matter</topic><topic>Dynamics</topic><topic>Flexibility</topic><topic>Lattice vibration</topic><topic>Lattices</topic><topic>LATTICES (CRYSTAL)</topic><topic>OXIDES</topic><topic>Rods</topic><topic>Thermal expansion</topic><topic>THERMAL EXPANSION COEFFICIENT</topic><topic>Vibration</topic><toplevel>online_resources</toplevel><creatorcontrib>Rimmer, Leila H N</creatorcontrib><creatorcontrib>Dove, Martin T</creatorcontrib><creatorcontrib>Winkler, Bjorn</creatorcontrib><creatorcontrib>Wilson, Dan J</creatorcontrib><creatorcontrib>Refson, Keith</creatorcontrib><creatorcontrib>Goodwin, Andrew L</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Copper Technical Reference Library</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. 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Low-frequency acoustic modes that are responsible for the NTE in this material correspond to vibrations of rigid O-Cu-O rods. There is also some small contribution from higher-frequency optic modes that correspond to rotations of rigid and near-rigid OCu sub(4) tetrahedra as well as of near-rigid O-Cu-O rods. The primary NTE mode also drives a ferroelastic phase transition at high pressure; our calculations predict this to be an orthorhombic structure with space group Pnnn.</abstract></addata></record> |
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subjects | Condensed matter Dynamics Flexibility Lattice vibration Lattices LATTICES (CRYSTAL) OXIDES Rods Thermal expansion THERMAL EXPANSION COEFFICIENT Vibration |
title | Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu sub(2) O |
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