Short-Range Order and Dynamics in Crystalline α-TeO2
The short-range order and dynamics in crystalline α-TeO2 have been investigated by neutron and X-ray total scattering and by Rietveld refinement of neutron diffraction data. The true lengths of the two bonds in a Te–O–Te bridge are 1.882(1) and 2.117(1) Å, and the high valence, 1.293, of the strong,...
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Veröffentlicht in: | Journal of physical chemistry. C 2012-02, Vol.116 (5), p.3707-3718 |
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description | The short-range order and dynamics in crystalline α-TeO2 have been investigated by neutron and X-ray total scattering and by Rietveld refinement of neutron diffraction data. The true lengths of the two bonds in a Te–O–Te bridge are 1.882(1) and 2.117(1) Å, and the high valence, 1.293, of the strong, short bond is balanced by the low valence, 0.686, of the weak, long bond. The root-mean-square (rms) thermal variation, 0.083(1) Å, in the long bond length is nearly twice the rms thermal variation, 0.048(1) Å, in the short bond length because the largest motion of both Te and O atoms is perpendicular to the short bonds. A bond-valence model for the thermal variation in bond lengths, in which both the average and the instantaneous positions of the atoms conform to bond-valence requirements, accounts closely for the observed distribution of Te–O distances in α-TeO2. This has important implications for the interpretation of diffraction experiments on tellurite glasses. |
doi_str_mv | 10.1021/jp207858x |
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C ; Holland, D</creator><creatorcontrib>Barney, E. R ; Hannon, A. C ; Holland, D</creatorcontrib><description>The short-range order and dynamics in crystalline α-TeO2 have been investigated by neutron and X-ray total scattering and by Rietveld refinement of neutron diffraction data. The true lengths of the two bonds in a Te–O–Te bridge are 1.882(1) and 2.117(1) Å, and the high valence, 1.293, of the strong, short bond is balanced by the low valence, 0.686, of the weak, long bond. The root-mean-square (rms) thermal variation, 0.083(1) Å, in the long bond length is nearly twice the rms thermal variation, 0.048(1) Å, in the short bond length because the largest motion of both Te and O atoms is perpendicular to the short bonds. A bond-valence model for the thermal variation in bond lengths, in which both the average and the instantaneous positions of the atoms conform to bond-valence requirements, accounts closely for the observed distribution of Te–O distances in α-TeO2. This has important implications for the interpretation of diffraction experiments on tellurite glasses.</description><identifier>ISSN: 1932-7447</identifier><identifier>EISSN: 1932-7455</identifier><identifier>DOI: 10.1021/jp207858x</identifier><language>eng</language><publisher>Columbus, OH: American Chemical Society</publisher><subject>C: Electron Transport, Optical and Electronic Devices, Hard Matter ; Condensed matter: structure, mechanical and thermal properties ; Exact sciences and technology ; Neutron diffraction and scattering ; Physics ; Single-crystal and powder diffraction ; Structure of solids and liquids; crystallography ; X-ray diffraction and scattering ; X-ray scattering (including small-angle scattering)</subject><ispartof>Journal of physical chemistry. 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C</creatorcontrib><creatorcontrib>Holland, D</creatorcontrib><title>Short-Range Order and Dynamics in Crystalline α-TeO2</title><title>Journal of physical chemistry. C</title><addtitle>J. Phys. Chem. C</addtitle><description>The short-range order and dynamics in crystalline α-TeO2 have been investigated by neutron and X-ray total scattering and by Rietveld refinement of neutron diffraction data. The true lengths of the two bonds in a Te–O–Te bridge are 1.882(1) and 2.117(1) Å, and the high valence, 1.293, of the strong, short bond is balanced by the low valence, 0.686, of the weak, long bond. The root-mean-square (rms) thermal variation, 0.083(1) Å, in the long bond length is nearly twice the rms thermal variation, 0.048(1) Å, in the short bond length because the largest motion of both Te and O atoms is perpendicular to the short bonds. A bond-valence model for the thermal variation in bond lengths, in which both the average and the instantaneous positions of the atoms conform to bond-valence requirements, accounts closely for the observed distribution of Te–O distances in α-TeO2. This has important implications for the interpretation of diffraction experiments on tellurite glasses.</description><subject>C: Electron Transport, Optical and Electronic Devices, Hard Matter</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Exact sciences and technology</subject><subject>Neutron diffraction and scattering</subject><subject>Physics</subject><subject>Single-crystal and powder diffraction</subject><subject>Structure of solids and liquids; crystallography</subject><subject>X-ray diffraction and scattering</subject><subject>X-ray scattering (including small-angle scattering)</subject><issn>1932-7447</issn><issn>1932-7455</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNpFkM1KxDAcxIMouK4efINcPEbz2TRHqZ-wUND1HP5NUm3pZktSwX0sX8RnsqKspxmGYfgxCJ0zeskoZ1f9yKkuVflxgBbMCE60VOpw76U-Ric595QqQZlYIPX8tk0TeYL4GnCdfEgYosc3uwibzmXcRVylXZ5gGLoY8NcnWYean6KjFoYczv50iV7ubtfVA1nV94_V9YoAk2oiTaG5kE1bOjBGi8aAB86NdgKELyTXfA6bolWcuRnaMV74IEpJJTRMlV4s0cXv7gjZwdAmiK7LdkzdBtLOcqULI4X574HLtt--pzhTWUbtzyd2_4n4BnpUUlM</recordid><startdate>20120209</startdate><enddate>20120209</enddate><creator>Barney, E. R</creator><creator>Hannon, A. C</creator><creator>Holland, D</creator><general>American Chemical Society</general><scope>IQODW</scope></search><sort><creationdate>20120209</creationdate><title>Short-Range Order and Dynamics in Crystalline α-TeO2</title><author>Barney, E. R ; Hannon, A. C ; Holland, D</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a145t-b67234bf8ca9973b9ada2297c3a3d6427273bb6f521c785c126de38404ab158d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>C: Electron Transport, Optical and Electronic Devices, Hard Matter</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Exact sciences and technology</topic><topic>Neutron diffraction and scattering</topic><topic>Physics</topic><topic>Single-crystal and powder diffraction</topic><topic>Structure of solids and liquids; crystallography</topic><topic>X-ray diffraction and scattering</topic><topic>X-ray scattering (including small-angle scattering)</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Barney, E. R</creatorcontrib><creatorcontrib>Hannon, A. C</creatorcontrib><creatorcontrib>Holland, D</creatorcontrib><collection>Pascal-Francis</collection><jtitle>Journal of physical chemistry. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Barney, E. R</au><au>Hannon, A. C</au><au>Holland, D</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Short-Range Order and Dynamics in Crystalline α-TeO2</atitle><jtitle>Journal of physical chemistry. C</jtitle><addtitle>J. Phys. Chem. C</addtitle><date>2012-02-09</date><risdate>2012</risdate><volume>116</volume><issue>5</issue><spage>3707</spage><epage>3718</epage><pages>3707-3718</pages><issn>1932-7447</issn><eissn>1932-7455</eissn><abstract>The short-range order and dynamics in crystalline α-TeO2 have been investigated by neutron and X-ray total scattering and by Rietveld refinement of neutron diffraction data. The true lengths of the two bonds in a Te–O–Te bridge are 1.882(1) and 2.117(1) Å, and the high valence, 1.293, of the strong, short bond is balanced by the low valence, 0.686, of the weak, long bond. The root-mean-square (rms) thermal variation, 0.083(1) Å, in the long bond length is nearly twice the rms thermal variation, 0.048(1) Å, in the short bond length because the largest motion of both Te and O atoms is perpendicular to the short bonds. A bond-valence model for the thermal variation in bond lengths, in which both the average and the instantaneous positions of the atoms conform to bond-valence requirements, accounts closely for the observed distribution of Te–O distances in α-TeO2. This has important implications for the interpretation of diffraction experiments on tellurite glasses.</abstract><cop>Columbus, OH</cop><pub>American Chemical Society</pub><doi>10.1021/jp207858x</doi><tpages>12</tpages></addata></record> |
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subjects | C: Electron Transport, Optical and Electronic Devices, Hard Matter Condensed matter: structure, mechanical and thermal properties Exact sciences and technology Neutron diffraction and scattering Physics Single-crystal and powder diffraction Structure of solids and liquids crystallography X-ray diffraction and scattering X-ray scattering (including small-angle scattering) |
title | Short-Range Order and Dynamics in Crystalline α-TeO2 |
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