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Structural transition at 225 K of the trinuclear Fe(III) heptanoate [Fe3O(O2CC6H13)6(H2O)3]NO3
The trinuclear iron (III) heptanoate [Fe30(O2CC6H13)6(H2O)3]NO3 compound is synthesized and studied by single crystal X-ray diffraction as a function of the temperature, also by Fe57 Mossbauer spectroscopy, electrochemical and magnetic measurements. Its thermal behavior is determined by DSC, TGA and...
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Published in: | Solid state sciences 2005-10, Vol.7 (10), p.1236-1246 |
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description | The trinuclear iron (III) heptanoate [Fe30(O2CC6H13)6(H2O)3]NO3 compound is synthesized and studied by single crystal X-ray diffraction as a function of the temperature, also by Fe57 Mossbauer spectroscopy, electrochemical and magnetic measurements. Its thermal behavior is determined by DSC, TGA and X-ray diffraction. The compound undergoes a structural phase transition at Ts = 225 K giving a superstructure of order two (above Ts: P -1, a = 11.1393(2) A, b = 14.2757(3) A, c = 18.2088(4) A, a = 80.607(1)DG, B = 84.175(l)DG, y = 83.464(1)DG; below Ts: P -1, a = 11.0122(2) A, b = 14.2723(3) A, c = 35.5222(7) A, a = 94.138(1)DG, 0 = 97.136(1)DG, y = 96.779(l)DG). The origin of the transition is interpreted as being due to a 60DG rotation of the nitrate groups of one sheet out of two of the lamellar structure. Analysis of the Fe57 Mossbauer spectra as a function of the temperature does not show electronic transition such as valence trapped phenoma below Ts. The compound has a paramagnetic behavior in the temperature range 300-2 K. A Heisenberg model of interaction based on triangular Fe(III) units of quantum S = 5/2 spins is used for simulating the variation of the susceptibility between room temperature and 2 K. |
doi_str_mv | 10.1016/j.solidstatesciences.2005.05.008 |
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I ; RABU, P ; SOUHASSOU, M ; MALAMAN, B ; STEINMETZ, J</creator><creatorcontrib>FRANCOIS, M ; SALEH, M. I ; RABU, P ; SOUHASSOU, M ; MALAMAN, B ; STEINMETZ, J</creatorcontrib><description>The trinuclear iron (III) heptanoate [Fe30(O2CC6H13)6(H2O)3]NO3 compound is synthesized and studied by single crystal X-ray diffraction as a function of the temperature, also by Fe57 Mossbauer spectroscopy, electrochemical and magnetic measurements. Its thermal behavior is determined by DSC, TGA and X-ray diffraction. The compound undergoes a structural phase transition at Ts = 225 K giving a superstructure of order two (above Ts: P -1, a = 11.1393(2) A, b = 14.2757(3) A, c = 18.2088(4) A, a = 80.607(1)DG, B = 84.175(l)DG, y = 83.464(1)DG; below Ts: P -1, a = 11.0122(2) A, b = 14.2723(3) A, c = 35.5222(7) A, a = 94.138(1)DG, 0 = 97.136(1)DG, y = 96.779(l)DG). The origin of the transition is interpreted as being due to a 60DG rotation of the nitrate groups of one sheet out of two of the lamellar structure. Analysis of the Fe57 Mossbauer spectra as a function of the temperature does not show electronic transition such as valence trapped phenoma below Ts. The compound has a paramagnetic behavior in the temperature range 300-2 K. A Heisenberg model of interaction based on triangular Fe(III) units of quantum S = 5/2 spins is used for simulating the variation of the susceptibility between room temperature and 2 K.</description><identifier>ISSN: 1293-2558</identifier><identifier>EISSN: 1873-3085</identifier><identifier>DOI: 10.1016/j.solidstatesciences.2005.05.008</identifier><language>eng</language><publisher>Paris: Elsevier</publisher><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Condensed matter: structure, mechanical and thermal properties ; Crystalline state (including molecular motions in solids) ; Diamagnetism, paramagnetism and superparamagnetism ; Exact sciences and technology ; Magnetic properties and materials ; Magnetic resonances and relaxations in condensed matter, mössbauer effect ; Mössbauer effect; other γ-ray spectroscopy ; Physics ; Structure of solids and liquids; crystallography ; Structure of specific crystalline solids ; Theory of crystal structure, crystal symmetry; calculations and modeling</subject><ispartof>Solid state sciences, 2005-10, Vol.7 (10), p.1236-1246</ispartof><rights>2006 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c336t-bcf444c5ff7eb06fd2362876af84ad6992a160a9eef3fe42a709f7ee52ce65a53</citedby><cites>FETCH-LOGICAL-c336t-bcf444c5ff7eb06fd2362876af84ad6992a160a9eef3fe42a709f7ee52ce65a53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=17142198$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>FRANCOIS, M</creatorcontrib><creatorcontrib>SALEH, M. 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The compound undergoes a structural phase transition at Ts = 225 K giving a superstructure of order two (above Ts: P -1, a = 11.1393(2) A, b = 14.2757(3) A, c = 18.2088(4) A, a = 80.607(1)DG, B = 84.175(l)DG, y = 83.464(1)DG; below Ts: P -1, a = 11.0122(2) A, b = 14.2723(3) A, c = 35.5222(7) A, a = 94.138(1)DG, 0 = 97.136(1)DG, y = 96.779(l)DG). The origin of the transition is interpreted as being due to a 60DG rotation of the nitrate groups of one sheet out of two of the lamellar structure. Analysis of the Fe57 Mossbauer spectra as a function of the temperature does not show electronic transition such as valence trapped phenoma below Ts. The compound has a paramagnetic behavior in the temperature range 300-2 K. A Heisenberg model of interaction based on triangular Fe(III) units of quantum S = 5/2 spins is used for simulating the variation of the susceptibility between room temperature and 2 K.</description><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Crystalline state (including molecular motions in solids)</subject><subject>Diamagnetism, paramagnetism and superparamagnetism</subject><subject>Exact sciences and technology</subject><subject>Magnetic properties and materials</subject><subject>Magnetic resonances and relaxations in condensed matter, mössbauer effect</subject><subject>Mössbauer effect; other γ-ray spectroscopy</subject><subject>Physics</subject><subject>Structure of solids and liquids; crystallography</subject><subject>Structure of specific crystalline solids</subject><subject>Theory of crystal structure, crystal symmetry; calculations and modeling</subject><issn>1293-2558</issn><issn>1873-3085</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNplkE9Lw0AQxYMoWKvfYS9Ke0jdP9nN5qYUa4vFHNST6DLdztKUmNTdzcFvb0oLHoQHMzCP95hfkowYnTDK1O12Etq6WocIEYOtsLEYJpxSOdmL6pNkwHQuUkG1PO13XoiUS6nPk4sQtpRSpfJskHy-RN_Z2HmoSfTQhCpWbUMgEs4leSKtI3GD_alqOlsjeDLD0WKxGJMN7iI0bV9P3mcoylHJp1M1Z2KsRnNejsXHcykukzMHdcCr4xwmb7OH1-k8XZaPi-n9MrVCqJiurMuyzErnclxR5dZcKK5zBU5nsFZFwYEpCgWiEw4zDjkteitKblFJkGKY3Bxyd7797jBE81UFi3UNDbZdMFwzJvqHe-PdwWh9G4JHZ3a--gL_Yxg1e7Bma_6DNXuwZi-q-4jrYxcEC7Xrqdkq_OXkLOOs0OIXTJ5-KQ</recordid><startdate>20051001</startdate><enddate>20051001</enddate><creator>FRANCOIS, M</creator><creator>SALEH, M. 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I ; RABU, P ; SOUHASSOU, M ; MALAMAN, B ; STEINMETZ, J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c336t-bcf444c5ff7eb06fd2362876af84ad6992a160a9eef3fe42a709f7ee52ce65a53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Crystalline state (including molecular motions in solids)</topic><topic>Diamagnetism, paramagnetism and superparamagnetism</topic><topic>Exact sciences and technology</topic><topic>Magnetic properties and materials</topic><topic>Magnetic resonances and relaxations in condensed matter, mössbauer effect</topic><topic>Mössbauer effect; other γ-ray spectroscopy</topic><topic>Physics</topic><topic>Structure of solids and liquids; crystallography</topic><topic>Structure of specific crystalline solids</topic><topic>Theory of crystal structure, crystal symmetry; calculations and modeling</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>FRANCOIS, M</creatorcontrib><creatorcontrib>SALEH, M. I</creatorcontrib><creatorcontrib>RABU, P</creatorcontrib><creatorcontrib>SOUHASSOU, M</creatorcontrib><creatorcontrib>MALAMAN, B</creatorcontrib><creatorcontrib>STEINMETZ, J</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Ceramic Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Solid state sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>FRANCOIS, M</au><au>SALEH, M. I</au><au>RABU, P</au><au>SOUHASSOU, M</au><au>MALAMAN, B</au><au>STEINMETZ, J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural transition at 225 K of the trinuclear Fe(III) heptanoate [Fe3O(O2CC6H13)6(H2O)3]NO3</atitle><jtitle>Solid state sciences</jtitle><date>2005-10-01</date><risdate>2005</risdate><volume>7</volume><issue>10</issue><spage>1236</spage><epage>1246</epage><pages>1236-1246</pages><issn>1293-2558</issn><eissn>1873-3085</eissn><abstract>The trinuclear iron (III) heptanoate [Fe30(O2CC6H13)6(H2O)3]NO3 compound is synthesized and studied by single crystal X-ray diffraction as a function of the temperature, also by Fe57 Mossbauer spectroscopy, electrochemical and magnetic measurements. Its thermal behavior is determined by DSC, TGA and X-ray diffraction. The compound undergoes a structural phase transition at Ts = 225 K giving a superstructure of order two (above Ts: P -1, a = 11.1393(2) A, b = 14.2757(3) A, c = 18.2088(4) A, a = 80.607(1)DG, B = 84.175(l)DG, y = 83.464(1)DG; below Ts: P -1, a = 11.0122(2) A, b = 14.2723(3) A, c = 35.5222(7) A, a = 94.138(1)DG, 0 = 97.136(1)DG, y = 96.779(l)DG). The origin of the transition is interpreted as being due to a 60DG rotation of the nitrate groups of one sheet out of two of the lamellar structure. Analysis of the Fe57 Mossbauer spectra as a function of the temperature does not show electronic transition such as valence trapped phenoma below Ts. The compound has a paramagnetic behavior in the temperature range 300-2 K. A Heisenberg model of interaction based on triangular Fe(III) units of quantum S = 5/2 spins is used for simulating the variation of the susceptibility between room temperature and 2 K.</abstract><cop>Paris</cop><pub>Elsevier</pub><doi>10.1016/j.solidstatesciences.2005.05.008</doi><tpages>11</tpages></addata></record> |
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subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Condensed matter: structure, mechanical and thermal properties Crystalline state (including molecular motions in solids) Diamagnetism, paramagnetism and superparamagnetism Exact sciences and technology Magnetic properties and materials Magnetic resonances and relaxations in condensed matter, mössbauer effect Mössbauer effect other γ-ray spectroscopy Physics Structure of solids and liquids crystallography Structure of specific crystalline solids Theory of crystal structure, crystal symmetry calculations and modeling |
title | Structural transition at 225 K of the trinuclear Fe(III) heptanoate [Fe3O(O2CC6H13)6(H2O)3]NO3 |
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