The Anharmonic Origin of the Giant Thermal Expansion of NaBr
All phonons in a single crystal of NaBr were measured by inelastic neutron scattering at temperatures of 10, 300 and 700 K. Even at 300 K the phonons, especially the longitudinal-optical (LO) phonons, showed large shifts in frequencies, and showed large broadenings in energy owing to anharmonicity....
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description | All phonons in a single crystal of NaBr were measured by inelastic neutron scattering at temperatures of 10, 300 and 700 K. Even at 300 K the phonons, especially the longitudinal-optical (LO) phonons, showed large shifts in frequencies, and showed large broadenings in energy owing to anharmonicity. Ab initio computations were first performed with the quasiharmonic approximation (QHA), in which the phonon frequencies depend only on \(V\), and on \(T\) only insofar as it alters \(V\) by thermal expansion. This QHA was an unqualified failure for predicting the temperature dependence of phonon frequencies, even 300 K, and the thermal expansion was in error by a factor of four. Ab initio computations that included both anharmonicity and quasiharmonicity successfully predicted both the temperature dependence of phonons and the large thermal expansion of NaBr. The frequencies of LO phonon modes decrease significantly with temperature owing to the real part of the phonon self-energy from explicit anhamonicity, originating from the cubic anharmonicity of nearest-neighbor Na-Br bonds. Anharmonicity is not a correction to the QHA predictions of thermal expansion and thermal phonon shifts, but dominates the behavior. |
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Even at 300 K the phonons, especially the longitudinal-optical (LO) phonons, showed large shifts in frequencies, and showed large broadenings in energy owing to anharmonicity. Ab initio computations were first performed with the quasiharmonic approximation (QHA), in which the phonon frequencies depend only on \(V\), and on \(T\) only insofar as it alters \(V\) by thermal expansion. This QHA was an unqualified failure for predicting the temperature dependence of phonon frequencies, even 300 K, and the thermal expansion was in error by a factor of four. Ab initio computations that included both anharmonicity and quasiharmonicity successfully predicted both the temperature dependence of phonons and the large thermal expansion of NaBr. The frequencies of LO phonon modes decrease significantly with temperature owing to the real part of the phonon self-energy from explicit anhamonicity, originating from the cubic anharmonicity of nearest-neighbor Na-Br bonds. 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Anharmonicity is not a correction to the QHA predictions of thermal expansion and thermal phonon shifts, but dominates the behavior.</description><subject>Anharmonicity</subject><subject>Inelastic scattering</subject><subject>Longitude</subject><subject>Neutron scattering</subject><subject>Neutrons</subject><subject>Phonons</subject><subject>Physics - Materials Science</subject><subject>Predictions</subject><subject>Single crystals</subject><subject>Sodium bromides</subject><subject>Temperature</subject><subject>Temperature dependence</subject><subject>Thermal expansion</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj01Lw0AURQdBsNT-AFcOuE58eTNvMgE3tdQqFLvJPky-7JRmEiep1H9vmrq6i3u43MPYQwSh1ETwbPzZ_oRRAkkIIiK4YTMUIgq0RLxji74_AACqGInEjL2k-4ov3d74pnW24Dtvv6zjbc2HsdhY4wY-Ir4xR74-d8b1tp3qT_Pq79ltbY59tfjPOUvf1unqPdjuNh-r5TYwhBSUosS60BWqROqEdK1I1LkqDFZJTqrGMocCKpBSxlEukxg1KtCkIkIhSxJz9nidndSyztvG-N_sophNiiPxdCU6336fqn7IDu3Ju_FThqhjLVWsSfwBNitROg</recordid><startdate>20190906</startdate><enddate>20190906</enddate><creator>Shen, Y</creator><creator>Saunders, C N</creator><creator>Bernal, C M</creator><creator>Abernathy, D L</creator><creator>Manley, M E</creator><creator>Fultz, B</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20190906</creationdate><title>The Anharmonic Origin of the Giant Thermal Expansion of NaBr</title><author>Shen, Y ; Saunders, C N ; Bernal, C M ; Abernathy, D L ; Manley, M E ; Fultz, B</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a525-d3d2fc8e26948958f653fb6ca2e9b56f2db0c0e044471b4972826085615234d53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Anharmonicity</topic><topic>Inelastic scattering</topic><topic>Longitude</topic><topic>Neutron scattering</topic><topic>Neutrons</topic><topic>Phonons</topic><topic>Physics - Materials Science</topic><topic>Predictions</topic><topic>Single crystals</topic><topic>Sodium bromides</topic><topic>Temperature</topic><topic>Temperature dependence</topic><topic>Thermal expansion</topic><toplevel>online_resources</toplevel><creatorcontrib>Shen, Y</creatorcontrib><creatorcontrib>Saunders, C N</creatorcontrib><creatorcontrib>Bernal, C M</creatorcontrib><creatorcontrib>Abernathy, D L</creatorcontrib><creatorcontrib>Manley, M E</creatorcontrib><creatorcontrib>Fultz, B</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shen, Y</au><au>Saunders, C N</au><au>Bernal, C M</au><au>Abernathy, D L</au><au>Manley, M E</au><au>Fultz, B</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Anharmonic Origin of the Giant Thermal Expansion of NaBr</atitle><jtitle>arXiv.org</jtitle><date>2019-09-06</date><risdate>2019</risdate><eissn>2331-8422</eissn><abstract>All phonons in a single crystal of NaBr were measured by inelastic neutron scattering at temperatures of 10, 300 and 700 K. Even at 300 K the phonons, especially the longitudinal-optical (LO) phonons, showed large shifts in frequencies, and showed large broadenings in energy owing to anharmonicity. Ab initio computations were first performed with the quasiharmonic approximation (QHA), in which the phonon frequencies depend only on \(V\), and on \(T\) only insofar as it alters \(V\) by thermal expansion. This QHA was an unqualified failure for predicting the temperature dependence of phonon frequencies, even 300 K, and the thermal expansion was in error by a factor of four. Ab initio computations that included both anharmonicity and quasiharmonicity successfully predicted both the temperature dependence of phonons and the large thermal expansion of NaBr. The frequencies of LO phonon modes decrease significantly with temperature owing to the real part of the phonon self-energy from explicit anhamonicity, originating from the cubic anharmonicity of nearest-neighbor Na-Br bonds. Anharmonicity is not a correction to the QHA predictions of thermal expansion and thermal phonon shifts, but dominates the behavior.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1909.03150</doi><oa>free_for_read</oa></addata></record> |
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subjects | Anharmonicity Inelastic scattering Longitude Neutron scattering Neutrons Phonons Physics - Materials Science Predictions Single crystals Sodium bromides Temperature Temperature dependence Thermal expansion |
title | The Anharmonic Origin of the Giant Thermal Expansion of NaBr |
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