Wing structure in the phase diagram of the Ising ferromagnet URhGe close to its tricritical point investigated by angle-resolved magnetization measurements
High-precision angle-resolved dc magnetization and magnetic torque studies were performed on a single-crystalline sample of URhGe, an orthorhombic Ising ferromagnet with the c axis being the magnetization easy axis, in order to investigate the phase diagram around the ferromagnetic (FM) reorientatio...
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Veröffentlicht in: | Physical review. B 2017-09, Vol.96 (9), Article 094411 |
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creator | Nakamura, Shota Sakakibara, Toshiro Shimizu, Yusei Kittaka, Shunichiro Kono, Yohei Haga, Yoshinori Pospíšil, Jiří Yamamoto, Etsuji |
description | High-precision angle-resolved dc magnetization and magnetic torque studies were performed on a single-crystalline sample of URhGe, an orthorhombic Ising ferromagnet with the c axis being the magnetization easy axis, in order to investigate the phase diagram around the ferromagnetic (FM) reorientation transition in a magnetic field near the b axis. We have clearly detected a first-order transition in both the magnetization and the magnetic torque at low temperatures, and determined detailed profiles of the wing structure of the three-dimensional T−Hb−Hc phase diagram, where Hc and Hb denote the field components along the c and the b axes, respectively. The quantum wing critical points are located at μ0Hc∼±1.1 T and μ0Hb∼13.5 T. Two second-order transition lines at the boundaries of the wing planes rapidly tend to approach each other with increasing temperature up to ∼3 K. Just at the zero conjugate field (Hc=0), however, a signature of the first-order transition can still be seen in the field derivative of the magnetization at ∼4 K, indicating that the tricritical point exists in a rather high temperature region above 4 K. This feature of the wing plane structure is consistent with the theoretical expectation that three second-order transition lines merge tangentially at the tricritical point. |
doi_str_mv | 10.1103/PhysRevB.96.094411 |
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We have clearly detected a first-order transition in both the magnetization and the magnetic torque at low temperatures, and determined detailed profiles of the wing structure of the three-dimensional T−Hb−Hc phase diagram, where Hc and Hb denote the field components along the c and the b axes, respectively. The quantum wing critical points are located at μ0Hc∼±1.1 T and μ0Hb∼13.5 T. Two second-order transition lines at the boundaries of the wing planes rapidly tend to approach each other with increasing temperature up to ∼3 K. Just at the zero conjugate field (Hc=0), however, a signature of the first-order transition can still be seen in the field derivative of the magnetization at ∼4 K, indicating that the tricritical point exists in a rather high temperature region above 4 K. This feature of the wing plane structure is consistent with the theoretical expectation that three second-order transition lines merge tangentially at the tricritical point.</description><identifier>ISSN: 2469-9950</identifier><identifier>EISSN: 2469-9969</identifier><identifier>DOI: 10.1103/PhysRevB.96.094411</identifier><language>eng</language><publisher>College Park: American Physical Society</publisher><subject>Ferromagnetism ; Ising model ; Magnetization ; Phase diagrams ; Single crystals ; Torque</subject><ispartof>Physical review. 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B</title><description>High-precision angle-resolved dc magnetization and magnetic torque studies were performed on a single-crystalline sample of URhGe, an orthorhombic Ising ferromagnet with the c axis being the magnetization easy axis, in order to investigate the phase diagram around the ferromagnetic (FM) reorientation transition in a magnetic field near the b axis. We have clearly detected a first-order transition in both the magnetization and the magnetic torque at low temperatures, and determined detailed profiles of the wing structure of the three-dimensional T−Hb−Hc phase diagram, where Hc and Hb denote the field components along the c and the b axes, respectively. The quantum wing critical points are located at μ0Hc∼±1.1 T and μ0Hb∼13.5 T. Two second-order transition lines at the boundaries of the wing planes rapidly tend to approach each other with increasing temperature up to ∼3 K. Just at the zero conjugate field (Hc=0), however, a signature of the first-order transition can still be seen in the field derivative of the magnetization at ∼4 K, indicating that the tricritical point exists in a rather high temperature region above 4 K. This feature of the wing plane structure is consistent with the theoretical expectation that three second-order transition lines merge tangentially at the tricritical point.</description><subject>Ferromagnetism</subject><subject>Ising model</subject><subject>Magnetization</subject><subject>Phase diagrams</subject><subject>Single crystals</subject><subject>Torque</subject><issn>2469-9950</issn><issn>2469-9969</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNo9kV9LwzAUxYsoOOa-gE8BnzuTNs1yH3X4ZzBQxsTHkmW3bUbb1CQbzK_il7Wz6tM9HH6ce-BE0TWjU8ZoevtaHf0KD_dTEFMKnDN2Fo0SLiAGEHD-rzN6GU2831FKmaAwozCKvt5NWxIf3F6HvUNiWhIqJF2lPJKtUaVTDbHFj7nwJ7ZA52yjyhYDeVtVT0h0bXs4WGKCJ8EZ7UwwWtWks6YNfeQBfTClCrglmyNRbVlj7NDb-tA7Q5T5VMHYljSofN-jwTb4q-iiULXHye8dR-vHh_X8OV6-PC3md8tYp5yFGDhuGcUEQDFRFCD1Zsa1AKH0hiVUpjzRVAmZSSl5WkAhZcYV760URKbTcXQzxHbOfuz7qvnO7l3bf8wTlqRMJmwGPZUMlHbWe4dF3jnTKHfMGc1PM-R_M-Qg8mGG9BvB4X_o</recordid><startdate>20170911</startdate><enddate>20170911</enddate><creator>Nakamura, Shota</creator><creator>Sakakibara, Toshiro</creator><creator>Shimizu, Yusei</creator><creator>Kittaka, Shunichiro</creator><creator>Kono, Yohei</creator><creator>Haga, Yoshinori</creator><creator>Pospíšil, Jiří</creator><creator>Yamamoto, Etsuji</creator><general>American Physical Society</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20170911</creationdate><title>Wing structure in the phase diagram of the Ising ferromagnet URhGe close to its tricritical point investigated by angle-resolved magnetization measurements</title><author>Nakamura, Shota ; Sakakibara, Toshiro ; Shimizu, Yusei ; Kittaka, Shunichiro ; Kono, Yohei ; Haga, Yoshinori ; Pospíšil, Jiří ; Yamamoto, Etsuji</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c341t-94ed10e299a16ff98cb74c696acb1208342c0a68588843f9f8854a40a63965c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Ferromagnetism</topic><topic>Ising model</topic><topic>Magnetization</topic><topic>Phase diagrams</topic><topic>Single crystals</topic><topic>Torque</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nakamura, Shota</creatorcontrib><creatorcontrib>Sakakibara, Toshiro</creatorcontrib><creatorcontrib>Shimizu, Yusei</creatorcontrib><creatorcontrib>Kittaka, Shunichiro</creatorcontrib><creatorcontrib>Kono, Yohei</creatorcontrib><creatorcontrib>Haga, Yoshinori</creatorcontrib><creatorcontrib>Pospíšil, Jiří</creatorcontrib><creatorcontrib>Yamamoto, Etsuji</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nakamura, Shota</au><au>Sakakibara, Toshiro</au><au>Shimizu, Yusei</au><au>Kittaka, Shunichiro</au><au>Kono, Yohei</au><au>Haga, Yoshinori</au><au>Pospíšil, Jiří</au><au>Yamamoto, Etsuji</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Wing structure in the phase diagram of the Ising ferromagnet URhGe close to its tricritical point investigated by angle-resolved magnetization measurements</atitle><jtitle>Physical review. B</jtitle><date>2017-09-11</date><risdate>2017</risdate><volume>96</volume><issue>9</issue><artnum>094411</artnum><issn>2469-9950</issn><eissn>2469-9969</eissn><abstract>High-precision angle-resolved dc magnetization and magnetic torque studies were performed on a single-crystalline sample of URhGe, an orthorhombic Ising ferromagnet with the c axis being the magnetization easy axis, in order to investigate the phase diagram around the ferromagnetic (FM) reorientation transition in a magnetic field near the b axis. We have clearly detected a first-order transition in both the magnetization and the magnetic torque at low temperatures, and determined detailed profiles of the wing structure of the three-dimensional T−Hb−Hc phase diagram, where Hc and Hb denote the field components along the c and the b axes, respectively. The quantum wing critical points are located at μ0Hc∼±1.1 T and μ0Hb∼13.5 T. Two second-order transition lines at the boundaries of the wing planes rapidly tend to approach each other with increasing temperature up to ∼3 K. Just at the zero conjugate field (Hc=0), however, a signature of the first-order transition can still be seen in the field derivative of the magnetization at ∼4 K, indicating that the tricritical point exists in a rather high temperature region above 4 K. This feature of the wing plane structure is consistent with the theoretical expectation that three second-order transition lines merge tangentially at the tricritical point.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevB.96.094411</doi></addata></record> |
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title | Wing structure in the phase diagram of the Ising ferromagnet URhGe close to its tricritical point investigated by angle-resolved magnetization measurements |
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