Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2O

The negative thermal expansion (NTE) mechanism in Cu2O has been characterized via mapping of different Cu2O 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...

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Main Authors: Rimmer, L, Dove, M, Winkler, B, Wilson, D, Refson, K, Goodwin, A
Format: Journal article
Language:English
Published: American Physical Society 2014
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author Rimmer, L
Dove, M
Winkler, B
Wilson, D
Refson, K
Goodwin, A
author_facet Rimmer, L
Dove, M
Winkler, B
Wilson, D
Refson, K
Goodwin, A
author_sort Rimmer, L
collection OXFORD
description The negative thermal expansion (NTE) mechanism in Cu2O has been characterized via mapping of different Cu2O 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 OCu4 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. © 2014 American Physical Society.
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spelling oxford-uuid:195d4cb2-4011-4993-8921-2f31dc4056782022-03-26T10:48:37ZFramework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2OJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:195d4cb2-4011-4993-8921-2f31dc405678EnglishSymplectic Elements at OxfordAmerican Physical Society2014Rimmer, LDove, MWinkler, BWilson, DRefson, KGoodwin, AThe negative thermal expansion (NTE) mechanism in Cu2O has been characterized via mapping of different Cu2O 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 OCu4 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. © 2014 American Physical Society.
spellingShingle Rimmer, L
Dove, M
Winkler, B
Wilson, D
Refson, K
Goodwin, A
Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2O
title Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2O
title_full Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2O
title_fullStr Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2O
title_full_unstemmed Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2O
title_short Framework flexibility and the negative thermal expansion mechanism of copper(I) oxide Cu2O
title_sort framework flexibility and the negative thermal expansion mechanism of copper i oxide cu2o
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