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Origin of field-induced discontinuous phase transitions in Nd2Fe17
Magnetic properties of a trigonal ferromagnet Nd2Fe17 have been studied on single crystals in steady (14 T) and pulsed (32 T) magnetic fields. The easy-magnetization direction lies close to the [120] axis, deviating from the basal plane by 2.9∘ (at T=5K). Of particular interest is the low-temperatur...
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Published in: | Physical review. B 2018-02, Vol.97 (5) |
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creator | Diop, L V B Kuz'min, M D Skokov, K P Skourski, Y Gutfleisch, O |
description | Magnetic properties of a trigonal ferromagnet Nd2Fe17 have been studied on single crystals in steady (14 T) and pulsed (32 T) magnetic fields. The easy-magnetization direction lies close to the [120] axis, deviating from the basal plane by 2.9∘ (at T=5K). Of particular interest is the low-temperature magnetization process along the high-symmetry axis [001], which is the hard direction. This process is discontinuous and involves two first-order phase transitions (FOMPs). One of them (at 20 T) is a symmetry FOMP similar to that observed in Sm2Fe17. The second transition (at 10.4 T) is unusual: as the magnetization turns abruptly toward the applied field, it also changes its azimuthal orientation (the angle φ) by 60∘. Both transitions can be reasonably accounted for by the presence of a significant sixth-order trigonal anisotropy term. |
doi_str_mv | 10.1103/PhysRevB.97.054406 |
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The easy-magnetization direction lies close to the [120] axis, deviating from the basal plane by 2.9∘ (at T=5K). Of particular interest is the low-temperature magnetization process along the high-symmetry axis [001], which is the hard direction. This process is discontinuous and involves two first-order phase transitions (FOMPs). One of them (at 20 T) is a symmetry FOMP similar to that observed in Sm2Fe17. The second transition (at 10.4 T) is unusual: as the magnetization turns abruptly toward the applied field, it also changes its azimuthal orientation (the angle φ) by 60∘. 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The easy-magnetization direction lies close to the [120] axis, deviating from the basal plane by 2.9∘ (at T=5K). Of particular interest is the low-temperature magnetization process along the high-symmetry axis [001], which is the hard direction. This process is discontinuous and involves two first-order phase transitions (FOMPs). One of them (at 20 T) is a symmetry FOMP similar to that observed in Sm2Fe17. The second transition (at 10.4 T) is unusual: as the magnetization turns abruptly toward the applied field, it also changes its azimuthal orientation (the angle φ) by 60∘. Both transitions can be reasonably accounted for by the presence of a significant sixth-order trigonal anisotropy term.</description><subject>Anisotropy</subject><subject>Basal plane</subject><subject>Ferromagnetism</subject><subject>Magnetic fields</subject><subject>Magnetic properties</subject><subject>Magnetism</subject><subject>Magnetization</subject><subject>Phase transitions</subject><subject>Single crystals</subject><subject>Symmetry</subject><issn>2469-9950</issn><issn>2469-9969</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNo9jcFKAzEURYMoWGp_wFXA9YwvyUvSLG2xKhQrouuSmSROSknqZEbw7x1QXJ27OfcQcs2gZgzE7Uv3XV7916o2ugaJCOqMzDgqUxmjzPn_lnBJFqUcAIApMBrMjKx2ffyIieZAQ_RHV8XkxtY76mJpcxpiGvNY6KmzxdOht6nEIeZU6OQ8O77xTF-Ri2CPxS_-OCfvm_u39WO13T08re-2VceZHiq0gTtpW68b3WKQrNGAVvOm9Wi4dFoKdMo2RnOxBK0QhXEIMiwnERkTc3Lz-3vq8-foy7A_5LFPU3LPGRdMM6WE-AH-jU2K</recordid><startdate>20180206</startdate><enddate>20180206</enddate><creator>Diop, L V B</creator><creator>Kuz'min, M D</creator><creator>Skokov, K P</creator><creator>Skourski, Y</creator><creator>Gutfleisch, O</creator><general>American Physical Society</general><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20180206</creationdate><title>Origin of field-induced discontinuous phase transitions in Nd2Fe17</title><author>Diop, L V B ; Kuz'min, M D ; Skokov, K P ; Skourski, Y ; Gutfleisch, O</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-h217t-4af2d5ace7b7c4f51b704a72bce4925d7534d6ab972380764439d405f8af24113</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Anisotropy</topic><topic>Basal plane</topic><topic>Ferromagnetism</topic><topic>Magnetic fields</topic><topic>Magnetic properties</topic><topic>Magnetism</topic><topic>Magnetization</topic><topic>Phase transitions</topic><topic>Single crystals</topic><topic>Symmetry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Diop, L V B</creatorcontrib><creatorcontrib>Kuz'min, M D</creatorcontrib><creatorcontrib>Skokov, K P</creatorcontrib><creatorcontrib>Skourski, Y</creatorcontrib><creatorcontrib>Gutfleisch, O</creatorcontrib><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. 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This process is discontinuous and involves two first-order phase transitions (FOMPs). One of them (at 20 T) is a symmetry FOMP similar to that observed in Sm2Fe17. The second transition (at 10.4 T) is unusual: as the magnetization turns abruptly toward the applied field, it also changes its azimuthal orientation (the angle φ) by 60∘. Both transitions can be reasonably accounted for by the presence of a significant sixth-order trigonal anisotropy term.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevB.97.054406</doi><oa>free_for_read</oa></addata></record> |
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subjects | Anisotropy Basal plane Ferromagnetism Magnetic fields Magnetic properties Magnetism Magnetization Phase transitions Single crystals Symmetry |
title | Origin of field-induced discontinuous phase transitions in Nd2Fe17 |
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