Exciton condensation and its influence on the specific heat
In rare earth compounds with localized 4f states the observation of bound 4f-hole-5d-electron states, excitons, is questionable. On the other hand the same compounds exhibit p–d excitons, which are derived from itinerant bands. In rare earth compounds, which exhibit intermediate valence, 4f–5d hybri...
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description | In rare earth compounds with localized 4f states the observation of bound 4f-hole-5d-electron states, excitons, is questionable. On the other hand the same compounds exhibit p–d excitons, which are derived from itinerant bands. In rare earth compounds, which exhibit intermediate valence, 4f–5d hybridization produces a narrow, several 10meV wide 4f band. Now 4f–5d excitons are possible and have been observed in TmSe0.45Te0.55 and similar compositions. The special band structure of these materials permits an enormous amount of excitons (≈1021cm−3), which condense in a first order transition at low temperatures and high pressure. This static and immense concentration of excitons dominates the heat conductivity and the thermal diffusivity and even exhibits the phenomenon of superfluidity in a solid. The measured specific heat shows that phonons couple to these excitons forming exciton polarons. |
doi_str_mv | 10.1016/j.physb.2012.09.018 |
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On the other hand the same compounds exhibit p–d excitons, which are derived from itinerant bands. In rare earth compounds, which exhibit intermediate valence, 4f–5d hybridization produces a narrow, several 10meV wide 4f band. Now 4f–5d excitons are possible and have been observed in TmSe0.45Te0.55 and similar compositions. The special band structure of these materials permits an enormous amount of excitons (≈1021cm−3), which condense in a first order transition at low temperatures and high pressure. This static and immense concentration of excitons dominates the heat conductivity and the thermal diffusivity and even exhibits the phenomenon of superfluidity in a solid. The measured specific heat shows that phonons couple to these excitons forming exciton polarons.</description><identifier>ISSN: 0921-4526</identifier><identifier>EISSN: 1873-2135</identifier><identifier>DOI: 10.1016/j.physb.2012.09.018</identifier><language>eng</language><publisher>Kidlington: Elsevier B.V</publisher><subject>Band structure of solids ; Bands ; Condensed matter ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Condensed matter: structure, mechanical and thermal properties ; Condensing ; Electron states ; Exact sciences and technology ; Excitation ; Exciton condensation ; Excitons and related phenomena ; Optical constants: refractive index, complex dielectric constant, absorption, reflection and transmission coefficients, emissivity ; Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation ; Optical properties of bulk materials and thin films ; Phonons ; Physics ; Rare earth compounds ; Specific heat ; Thermal conductivity ; Thermal expansion; thermomechanical effects and density ; Thermal properties of condensed matter ; Thermal properties of crystalline solids</subject><ispartof>Physica. 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B, Condensed matter</title><description>In rare earth compounds with localized 4f states the observation of bound 4f-hole-5d-electron states, excitons, is questionable. On the other hand the same compounds exhibit p–d excitons, which are derived from itinerant bands. In rare earth compounds, which exhibit intermediate valence, 4f–5d hybridization produces a narrow, several 10meV wide 4f band. Now 4f–5d excitons are possible and have been observed in TmSe0.45Te0.55 and similar compositions. The special band structure of these materials permits an enormous amount of excitons (≈1021cm−3), which condense in a first order transition at low temperatures and high pressure. This static and immense concentration of excitons dominates the heat conductivity and the thermal diffusivity and even exhibits the phenomenon of superfluidity in a solid. The measured specific heat shows that phonons couple to these excitons forming exciton polarons.</description><subject>Band structure of solids</subject><subject>Bands</subject><subject>Condensed matter</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Condensing</subject><subject>Electron states</subject><subject>Exact sciences and technology</subject><subject>Excitation</subject><subject>Exciton condensation</subject><subject>Excitons and related phenomena</subject><subject>Optical constants: refractive index, complex dielectric constant, absorption, reflection and transmission coefficients, emissivity</subject><subject>Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation</subject><subject>Optical properties of bulk materials and thin films</subject><subject>Phonons</subject><subject>Physics</subject><subject>Rare earth compounds</subject><subject>Specific heat</subject><subject>Thermal conductivity</subject><subject>Thermal expansion; thermomechanical effects and density</subject><subject>Thermal properties of condensed matter</subject><subject>Thermal properties of crystalline solids</subject><issn>0921-4526</issn><issn>1873-2135</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNp9kD1PwzAQhi0EEiXwC1iyILEk-OzEiYUYUFU-pEosMFuu7aiuUifYLqL_HodWjNxyuq_37h6ErgGXgIHdbcpxvQ-rkmAgJeYlhvYEzaBtaEGA1qdohjmBoqoJO0cXIWxwMmhghu4X38rGweVqcNq4IKNNgXQ6tzHk1nX9zjhl8pSMa5OH0SjbWZWvjYyX6KyTfTBXR5-hj6fF-_ylWL49v84fl4WqKIkFqVeAcUcrKXlTV5TShlZaUuCUcQOaMcqYaqlk0FQt55ik-ooB4QwrXmuaoduD7uiHz50JUWxtUKbvpTPDLgigrAZoJ-UM0UOr8kMI3nRi9HYr_V4AFhMqsRG_qMSESmAuEqo0dXNcIIOSfeelUzb8jRLGWkzS5Rl6OPSZ9O2XNV4EZSc82nqjotCD_XfPD6aWfVI</recordid><startdate>20130101</startdate><enddate>20130101</enddate><creator>Wachter, P.</creator><creator>Bucher, B.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20130101</creationdate><title>Exciton condensation and its influence on the specific heat</title><author>Wachter, P. ; Bucher, B.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c432t-25b100f34aa9754333734da319369e1d66366c83a617489902734b612960c95d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Band structure of solids</topic><topic>Bands</topic><topic>Condensed matter</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Condensing</topic><topic>Electron states</topic><topic>Exact sciences and technology</topic><topic>Excitation</topic><topic>Exciton condensation</topic><topic>Excitons and related phenomena</topic><topic>Optical constants: refractive index, complex dielectric constant, absorption, reflection and transmission coefficients, emissivity</topic><topic>Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation</topic><topic>Optical properties of bulk materials and thin films</topic><topic>Phonons</topic><topic>Physics</topic><topic>Rare earth compounds</topic><topic>Specific heat</topic><topic>Thermal conductivity</topic><topic>Thermal expansion; thermomechanical effects and density</topic><topic>Thermal properties of condensed matter</topic><topic>Thermal properties of crystalline solids</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wachter, P.</creatorcontrib><creatorcontrib>Bucher, B.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica. 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Now 4f–5d excitons are possible and have been observed in TmSe0.45Te0.55 and similar compositions. The special band structure of these materials permits an enormous amount of excitons (≈1021cm−3), which condense in a first order transition at low temperatures and high pressure. This static and immense concentration of excitons dominates the heat conductivity and the thermal diffusivity and even exhibits the phenomenon of superfluidity in a solid. The measured specific heat shows that phonons couple to these excitons forming exciton polarons.</abstract><cop>Kidlington</cop><pub>Elsevier B.V</pub><doi>10.1016/j.physb.2012.09.018</doi><tpages>7</tpages></addata></record> |
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subjects | Band structure of solids Bands Condensed matter Condensed matter: electronic structure, electrical, magnetic, and optical properties Condensed matter: structure, mechanical and thermal properties Condensing Electron states Exact sciences and technology Excitation Exciton condensation Excitons and related phenomena Optical constants: refractive index, complex dielectric constant, absorption, reflection and transmission coefficients, emissivity Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation Optical properties of bulk materials and thin films Phonons Physics Rare earth compounds Specific heat Thermal conductivity Thermal expansion thermomechanical effects and density Thermal properties of condensed matter Thermal properties of crystalline solids |
title | Exciton condensation and its influence on the specific heat |
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