Observation of a metamagnetic transition in the 5f heavy-fermion compound UNi2Al3: Magnetization studies up to 90 T for single-crystalline U(Pd1−xNix)2Al3
We report an observation of metamagnetism in the 5f-electron heavy-fermion antiferromagnets UNi2Al3 at 78 T and U(Pd1−xNix)2Al3 at 30 T (42 T) for x=0.5 (x=0.75) using single-crystalline samples. The magnetization curves for U(Pd1−xNix)2Al3 (x=0.5 and 0.75) show a sharp increase at the metamagnetic...
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creator | Mochidzuki, Kenji Shimizu, Yusei Kondo, Akihiro Matsuo, Akira Li, Dexin Aoki, Dai Homma, Yoshiya Honda, Fuminori Flouquet, Jacques Nakamura, Daisuke Takeyama, Shojiro Kindo, Koichi |
description | We report an observation of metamagnetism in the 5f-electron heavy-fermion antiferromagnets UNi2Al3 at 78 T and U(Pd1−xNix)2Al3 at 30 T (42 T) for x=0.5 (x=0.75) using single-crystalline samples. The magnetization curves for U(Pd1−xNix)2Al3 (x=0.5 and 0.75) show a sharp increase at the metamagnetic transition (MMT) field Bm, strongly indicating their first-order nature. The obtained B−T phase diagram for x=0.5 suggests the possible presence of the tricritical point, while the MMT still occurs at high temperatures above TN from paramagnetic to polarized-paramagnetic states as a crossover. The results indicate that the antiferromagnetic order is closely connected to the MMT in U(Pd1−xNix)2Al3, but the metamagnetic behavior cannot be explained by the conventional spin flip of antiferromagnetic ordered moments. Our data for U(Pd1−xNix)2Al3 have revealed an empirical linear relation of Bm(x)∝Tχmax(x) and a scaling behavior in magnetic susceptibility of χ(T/Tχmax)/χmax, where Tχmax is the temperature of the susceptibility maximum [χmax≡χ(Tχmax)]. Importantly, the critical value of the magnetic polarization at the MMT Mcr is roughly unchanged, although the value of susceptibility is notably suppressed with increasing x. |
doi_str_mv | 10.1103/PhysRevB.100.165137 |
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The magnetization curves for U(Pd1−xNix)2Al3 (x=0.5 and 0.75) show a sharp increase at the metamagnetic transition (MMT) field Bm, strongly indicating their first-order nature. The obtained B−T phase diagram for x=0.5 suggests the possible presence of the tricritical point, while the MMT still occurs at high temperatures above TN from paramagnetic to polarized-paramagnetic states as a crossover. The results indicate that the antiferromagnetic order is closely connected to the MMT in U(Pd1−xNix)2Al3, but the metamagnetic behavior cannot be explained by the conventional spin flip of antiferromagnetic ordered moments. Our data for U(Pd1−xNix)2Al3 have revealed an empirical linear relation of Bm(x)∝Tχmax(x) and a scaling behavior in magnetic susceptibility of χ(T/Tχmax)/χmax, where Tχmax is the temperature of the susceptibility maximum [χmax≡χ(Tχmax)]. Importantly, the critical value of the magnetic polarization at the MMT Mcr is roughly unchanged, although the value of susceptibility is notably suppressed with increasing x.</description><identifier>ISSN: 2469-9950</identifier><identifier>EISSN: 2469-9969</identifier><identifier>DOI: 10.1103/PhysRevB.100.165137</identifier><language>eng</language><publisher>College Park: American Physical Society</publisher><subject>Antiferromagnetism ; Crystal structure ; Crystallinity ; Fermions ; Magnetic permeability ; Magnetism ; Magnetization ; Magnetization curves ; Phase diagrams ; Single crystals</subject><ispartof>Physical review. 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B</title><description>We report an observation of metamagnetism in the 5f-electron heavy-fermion antiferromagnets UNi2Al3 at 78 T and U(Pd1−xNix)2Al3 at 30 T (42 T) for x=0.5 (x=0.75) using single-crystalline samples. The magnetization curves for U(Pd1−xNix)2Al3 (x=0.5 and 0.75) show a sharp increase at the metamagnetic transition (MMT) field Bm, strongly indicating their first-order nature. The obtained B−T phase diagram for x=0.5 suggests the possible presence of the tricritical point, while the MMT still occurs at high temperatures above TN from paramagnetic to polarized-paramagnetic states as a crossover. The results indicate that the antiferromagnetic order is closely connected to the MMT in U(Pd1−xNix)2Al3, but the metamagnetic behavior cannot be explained by the conventional spin flip of antiferromagnetic ordered moments. Our data for U(Pd1−xNix)2Al3 have revealed an empirical linear relation of Bm(x)∝Tχmax(x) and a scaling behavior in magnetic susceptibility of χ(T/Tχmax)/χmax, where Tχmax is the temperature of the susceptibility maximum [χmax≡χ(Tχmax)]. Importantly, the critical value of the magnetic polarization at the MMT Mcr is roughly unchanged, although the value of susceptibility is notably suppressed with increasing x.</description><subject>Antiferromagnetism</subject><subject>Crystal structure</subject><subject>Crystallinity</subject><subject>Fermions</subject><subject>Magnetic permeability</subject><subject>Magnetism</subject><subject>Magnetization</subject><subject>Magnetization curves</subject><subject>Phase diagrams</subject><subject>Single crystals</subject><issn>2469-9950</issn><issn>2469-9969</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNo9kEtOwzAYhC0EElXpCdhYYgOLFDuO05hdQbyk0laoXVd-pXWV2CF2qpYTsGbN6TgJKUWsZjSj__ulAeAcoz7GiFxPVzv_qje3fYzaJKWYDI5AJ05SFjGWsuN_T9Ep6Hm_RgjhFLEBYh3wNRFe1xsejLPQ5ZDDUgde8qXVwUgYam69-S2NhWGlIc3hSvPNLsp1Xe5z6crKNVbB-djEw4LcwJfD9fsB6kOjjPawqWBwkCE4g7mroTd2WehI1jsfeFEYq-H8cqrw98fndmy2V3vUGTjJeeF170-7YP5wP7t7ikaTx-e74SiqMCYhojLhkigtGJJcC9qO0jqpRJYolSsZk1hoirI4zmSeKiGkSNGAkgwliRIoJl1wceBWtXtrtA-LtWtq275cxASnCaY0Y-QHQqxv3w</recordid><startdate>20191023</startdate><enddate>20191023</enddate><creator>Mochidzuki, Kenji</creator><creator>Shimizu, Yusei</creator><creator>Kondo, Akihiro</creator><creator>Matsuo, Akira</creator><creator>Li, Dexin</creator><creator>Aoki, Dai</creator><creator>Homma, Yoshiya</creator><creator>Honda, Fuminori</creator><creator>Flouquet, Jacques</creator><creator>Nakamura, Daisuke</creator><creator>Takeyama, Shojiro</creator><creator>Kindo, Koichi</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>20191023</creationdate><title>Observation of a metamagnetic transition in the 5f heavy-fermion compound UNi2Al3: Magnetization studies up to 90 T for single-crystalline U(Pd1−xNix)2Al3</title><author>Mochidzuki, Kenji ; Shimizu, Yusei ; Kondo, Akihiro ; Matsuo, Akira ; Li, Dexin ; Aoki, Dai ; Homma, Yoshiya ; Honda, Fuminori ; Flouquet, Jacques ; Nakamura, Daisuke ; Takeyama, Shojiro ; Kindo, Koichi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p113t-5c4ac3deb90caeb510390ccdb84ddfdc232be508228cf6dbbcb607538044db023</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Antiferromagnetism</topic><topic>Crystal structure</topic><topic>Crystallinity</topic><topic>Fermions</topic><topic>Magnetic permeability</topic><topic>Magnetism</topic><topic>Magnetization</topic><topic>Magnetization curves</topic><topic>Phase diagrams</topic><topic>Single crystals</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mochidzuki, Kenji</creatorcontrib><creatorcontrib>Shimizu, Yusei</creatorcontrib><creatorcontrib>Kondo, Akihiro</creatorcontrib><creatorcontrib>Matsuo, Akira</creatorcontrib><creatorcontrib>Li, Dexin</creatorcontrib><creatorcontrib>Aoki, Dai</creatorcontrib><creatorcontrib>Homma, Yoshiya</creatorcontrib><creatorcontrib>Honda, Fuminori</creatorcontrib><creatorcontrib>Flouquet, Jacques</creatorcontrib><creatorcontrib>Nakamura, Daisuke</creatorcontrib><creatorcontrib>Takeyama, Shojiro</creatorcontrib><creatorcontrib>Kindo, Koichi</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. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mochidzuki, Kenji</au><au>Shimizu, Yusei</au><au>Kondo, Akihiro</au><au>Matsuo, Akira</au><au>Li, Dexin</au><au>Aoki, Dai</au><au>Homma, Yoshiya</au><au>Honda, Fuminori</au><au>Flouquet, Jacques</au><au>Nakamura, Daisuke</au><au>Takeyama, Shojiro</au><au>Kindo, Koichi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Observation of a metamagnetic transition in the 5f heavy-fermion compound UNi2Al3: Magnetization studies up to 90 T for single-crystalline U(Pd1−xNix)2Al3</atitle><jtitle>Physical review. B</jtitle><date>2019-10-23</date><risdate>2019</risdate><volume>100</volume><issue>16</issue><issn>2469-9950</issn><eissn>2469-9969</eissn><abstract>We report an observation of metamagnetism in the 5f-electron heavy-fermion antiferromagnets UNi2Al3 at 78 T and U(Pd1−xNix)2Al3 at 30 T (42 T) for x=0.5 (x=0.75) using single-crystalline samples. The magnetization curves for U(Pd1−xNix)2Al3 (x=0.5 and 0.75) show a sharp increase at the metamagnetic transition (MMT) field Bm, strongly indicating their first-order nature. The obtained B−T phase diagram for x=0.5 suggests the possible presence of the tricritical point, while the MMT still occurs at high temperatures above TN from paramagnetic to polarized-paramagnetic states as a crossover. The results indicate that the antiferromagnetic order is closely connected to the MMT in U(Pd1−xNix)2Al3, but the metamagnetic behavior cannot be explained by the conventional spin flip of antiferromagnetic ordered moments. Our data for U(Pd1−xNix)2Al3 have revealed an empirical linear relation of Bm(x)∝Tχmax(x) and a scaling behavior in magnetic susceptibility of χ(T/Tχmax)/χmax, where Tχmax is the temperature of the susceptibility maximum [χmax≡χ(Tχmax)]. Importantly, the critical value of the magnetic polarization at the MMT Mcr is roughly unchanged, although the value of susceptibility is notably suppressed with increasing x.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevB.100.165137</doi></addata></record> |
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title | Observation of a metamagnetic transition in the 5f heavy-fermion compound UNi2Al3: Magnetization studies up to 90 T for single-crystalline U(Pd1−xNix)2Al3 |
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