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Evolution of magnetic properties in the normal spinel solid solution Mg(1-x)Cu(x)Cr2O4
We examine the evolution of magnetic properties in the normal spinel oxides Mg(1-x)Cu(x)Cr2O4 using magnetization and heat capacity measurements. The end-member compounds of the solid solution series have been studied in some detail because of their very interesting magnetic behavior. MgCr2O4 is a h...
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description | We examine the evolution of magnetic properties in the normal spinel oxides Mg(1-x)Cu(x)Cr2O4 using magnetization and heat capacity measurements. The end-member compounds of the solid solution series have been studied in some detail because of their very interesting magnetic behavior. MgCr2O4 is a highly frustrated system that undergoes a first order structural transition at its antiferromagnetic ordering temperature. CuCr2O4 is tetragonal at room temperature as a result of Jahn-Teller active tetrahedral Cu^2+ and undergoes a magnetic transition at 135 K. Substitution of magnetic cations for diamagnetic Mg^2+ on the tetrahedral A site in the compositional series Mg(1-x)Cu(x)Cr2O4 dramatically affects magnetic behavior. In the composition range 0 < x < 0.3, the compounds are antiferromagnetic. A sharp peak observed at 12.5K in the heat capacity of MgCr2O4 corresponding to a magnetically driven first order structural transition is suppressed even for small x suggesting glassy disorder. Uncompensated magnetism - with open magnetization loops - develops for samples in the x range 0.43 < x < 1. Multiple magnetic ordering temperatures and large coercive fields emerge in the intermediate composition range 0.43 < x < 0.47. The Neel temperature increases with increasing x across the series while the value of the Curie-Weiss Theta decreases. A magnetic temperature-composition phase diagram of the solid solution series is presented. |
doi_str_mv | 10.48550/arxiv.1110.1662 |
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The end-member compounds of the solid solution series have been studied in some detail because of their very interesting magnetic behavior. MgCr2O4 is a highly frustrated system that undergoes a first order structural transition at its antiferromagnetic ordering temperature. CuCr2O4 is tetragonal at room temperature as a result of Jahn-Teller active tetrahedral Cu^2+ and undergoes a magnetic transition at 135 K. Substitution of magnetic cations for diamagnetic Mg^2+ on the tetrahedral A site in the compositional series Mg(1-x)Cu(x)Cr2O4 dramatically affects magnetic behavior. In the composition range 0 < x < 0.3, the compounds are antiferromagnetic. A sharp peak observed at 12.5K in the heat capacity of MgCr2O4 corresponding to a magnetically driven first order structural transition is suppressed even for small x suggesting glassy disorder. Uncompensated magnetism - with open magnetization loops - develops for samples in the x range 0.43 < x < 1. Multiple magnetic ordering temperatures and large coercive fields emerge in the intermediate composition range 0.43 < x < 0.47. The Neel temperature increases with increasing x across the series while the value of the Curie-Weiss Theta decreases. A magnetic temperature-composition phase diagram of the solid solution series is presented.]]></description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1110.1662</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Antiferromagnetism ; Coercivity ; Composition ; Copper ; Curie temperature ; Diamagnetism ; Evolution ; Jahn-Teller effect ; Magnesium ; Magnetic properties ; Magnetic transitions ; Magnetism ; Magnetization ; Neel temperature ; Phase diagrams ; Solid solutions ; Specific heat ; Spinel ; Temperature</subject><ispartof>arXiv.org, 2011-10</ispartof><rights>2011. 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The end-member compounds of the solid solution series have been studied in some detail because of their very interesting magnetic behavior. MgCr2O4 is a highly frustrated system that undergoes a first order structural transition at its antiferromagnetic ordering temperature. CuCr2O4 is tetragonal at room temperature as a result of Jahn-Teller active tetrahedral Cu^2+ and undergoes a magnetic transition at 135 K. Substitution of magnetic cations for diamagnetic Mg^2+ on the tetrahedral A site in the compositional series Mg(1-x)Cu(x)Cr2O4 dramatically affects magnetic behavior. In the composition range 0 < x < 0.3, the compounds are antiferromagnetic. A sharp peak observed at 12.5K in the heat capacity of MgCr2O4 corresponding to a magnetically driven first order structural transition is suppressed even for small x suggesting glassy disorder. Uncompensated magnetism - with open magnetization loops - develops for samples in the x range 0.43 < x < 1. Multiple magnetic ordering temperatures and large coercive fields emerge in the intermediate composition range 0.43 < x < 0.47. The Neel temperature increases with increasing x across the series while the value of the Curie-Weiss Theta decreases. A magnetic temperature-composition phase diagram of the solid solution series is presented.]]></description><subject>Antiferromagnetism</subject><subject>Coercivity</subject><subject>Composition</subject><subject>Copper</subject><subject>Curie temperature</subject><subject>Diamagnetism</subject><subject>Evolution</subject><subject>Jahn-Teller effect</subject><subject>Magnesium</subject><subject>Magnetic properties</subject><subject>Magnetic transitions</subject><subject>Magnetism</subject><subject>Magnetization</subject><subject>Neel temperature</subject><subject>Phase diagrams</subject><subject>Solid solutions</subject><subject>Specific heat</subject><subject>Spinel</subject><subject>Temperature</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNotjktrAjEUhUOhULHuuwx0Yxdjk5unyyL2ARY30q0kJtrImEyTGfHnN8Vuzsc53MdB6IGSGddCkGeTL-E8o7QGVEq4QSNgjDaaA9yhSSlHQghIBUKwEfpanlM79CFFnPb4ZA7R92GHu5w6n_vgCw4R998ex5RPpsWlC9FXpDa4P72ufh6mtLk8LYZplQxrfo9u96YtfvLPMdq8LjeL92a1fvtYvKwaIyhrGLVAufFypwkAE646zbUC5bQ1so5Yq602TCtuFbg5IZQJ5Z2bW8sJsDF6vJ6tfX8GX_rtMQ051o9bIFoKoYhi7BcsbFBm</recordid><startdate>20111007</startdate><enddate>20111007</enddate><creator>Kemei, Moureen C</creator><creator>Moffitt, Stephanie L</creator><creator>Shoemaker, Daniel P</creator><creator>Seshadri, Ram</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></search><sort><creationdate>20111007</creationdate><title>Evolution of magnetic properties in the normal spinel solid solution Mg(1-x)Cu(x)Cr2O4</title><author>Kemei, Moureen C ; Moffitt, Stephanie L ; Shoemaker, Daniel P ; Seshadri, Ram</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a513-31b214ae6c802235d214848727d8ba6513bb8b8a3874b72d9001357edd9bb4023</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Antiferromagnetism</topic><topic>Coercivity</topic><topic>Composition</topic><topic>Copper</topic><topic>Curie temperature</topic><topic>Diamagnetism</topic><topic>Evolution</topic><topic>Jahn-Teller effect</topic><topic>Magnesium</topic><topic>Magnetic properties</topic><topic>Magnetic transitions</topic><topic>Magnetism</topic><topic>Magnetization</topic><topic>Neel temperature</topic><topic>Phase diagrams</topic><topic>Solid solutions</topic><topic>Specific heat</topic><topic>Spinel</topic><topic>Temperature</topic><toplevel>online_resources</toplevel><creatorcontrib>Kemei, Moureen C</creatorcontrib><creatorcontrib>Moffitt, Stephanie L</creatorcontrib><creatorcontrib>Shoemaker, Daniel P</creatorcontrib><creatorcontrib>Seshadri, Ram</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>ProQuest - 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><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kemei, Moureen C</au><au>Moffitt, Stephanie L</au><au>Shoemaker, Daniel P</au><au>Seshadri, Ram</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Evolution of magnetic properties in the normal spinel solid solution Mg(1-x)Cu(x)Cr2O4</atitle><jtitle>arXiv.org</jtitle><date>2011-10-07</date><risdate>2011</risdate><eissn>2331-8422</eissn><abstract><![CDATA[We examine the evolution of magnetic properties in the normal spinel oxides Mg(1-x)Cu(x)Cr2O4 using magnetization and heat capacity measurements. The end-member compounds of the solid solution series have been studied in some detail because of their very interesting magnetic behavior. MgCr2O4 is a highly frustrated system that undergoes a first order structural transition at its antiferromagnetic ordering temperature. CuCr2O4 is tetragonal at room temperature as a result of Jahn-Teller active tetrahedral Cu^2+ and undergoes a magnetic transition at 135 K. Substitution of magnetic cations for diamagnetic Mg^2+ on the tetrahedral A site in the compositional series Mg(1-x)Cu(x)Cr2O4 dramatically affects magnetic behavior. In the composition range 0 < x < 0.3, the compounds are antiferromagnetic. A sharp peak observed at 12.5K in the heat capacity of MgCr2O4 corresponding to a magnetically driven first order structural transition is suppressed even for small x suggesting glassy disorder. Uncompensated magnetism - with open magnetization loops - develops for samples in the x range 0.43 < x < 1. Multiple magnetic ordering temperatures and large coercive fields emerge in the intermediate composition range 0.43 < x < 0.47. The Neel temperature increases with increasing x across the series while the value of the Curie-Weiss Theta decreases. A magnetic temperature-composition phase diagram of the solid solution series is presented.]]></abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1110.1662</doi><oa>free_for_read</oa></addata></record> |
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subjects | Antiferromagnetism Coercivity Composition Copper Curie temperature Diamagnetism Evolution Jahn-Teller effect Magnesium Magnetic properties Magnetic transitions Magnetism Magnetization Neel temperature Phase diagrams Solid solutions Specific heat Spinel Temperature |
title | Evolution of magnetic properties in the normal spinel solid solution Mg(1-x)Cu(x)Cr2O4 |
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