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Specific heat of field-dependent magnetic orderings in HoNi2B2C
We have investigated the low-temperature specific heat of HoNi2B2C down to T = 1 K in various magnetic fields from 0 T to 5 T. At zero field, the specific heat exhibits a large peak at TN = 5.1 K, which is due to commensurate antiferromagnetic ordering, and other smaller peak at T1 = 5.5 K, which is...
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Published in: | Journal of the Physical Society of Japan 2001-10, Vol.70 (10), p.3037-3041 |
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container_title | Journal of the Physical Society of Japan |
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creator | CHOI, Jae-Hyuk DOH, Hyeonjin CHOI, Eun-Mi KIM, Heon-Jung LEE, Sung-Ik YAMAMOTO, Tatsuharu KAWAE, Tatsuya TAKEDA, Kazuyoshi |
description | We have investigated the low-temperature specific heat of HoNi2B2C down to T = 1 K in various magnetic fields from 0 T to 5 T. At zero field, the specific heat exhibits a large peak at TN = 5.1 K, which is due to commensurate antiferromagnetic ordering, and other smaller peak at T1 = 5.5 K, which is related to incommensurate ordering. As the field is increased up to 0.5 T, the first peak broadens and moves to a lower temperature, while the other peak at T1 moves to a higher temperature, which indicates that the phase between TN and T1 is more favored in magnetic fields. Among possible candidates for the phase, the a-axis modulation phase, which is an extension of a low temperature metamagnetic state, is the most probable. In the high-field region above 1 T, the two-peak feature is replaced by a broad-hill one that fades away with increasing fields, which is the typical smearing feature of the magnetic order at high fields. |
doi_str_mv | 10.1143/JPSJ.70.3037 |
format | article |
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At zero field, the specific heat exhibits a large peak at TN = 5.1 K, which is due to commensurate antiferromagnetic ordering, and other smaller peak at T1 = 5.5 K, which is related to incommensurate ordering. As the field is increased up to 0.5 T, the first peak broadens and moves to a lower temperature, while the other peak at T1 moves to a higher temperature, which indicates that the phase between TN and T1 is more favored in magnetic fields. Among possible candidates for the phase, the a-axis modulation phase, which is an extension of a low temperature metamagnetic state, is the most probable. 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At zero field, the specific heat exhibits a large peak at TN = 5.1 K, which is due to commensurate antiferromagnetic ordering, and other smaller peak at T1 = 5.5 K, which is related to incommensurate ordering. As the field is increased up to 0.5 T, the first peak broadens and moves to a lower temperature, while the other peak at T1 moves to a higher temperature, which indicates that the phase between TN and T1 is more favored in magnetic fields. Among possible candidates for the phase, the a-axis modulation phase, which is an extension of a low temperature metamagnetic state, is the most probable. 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DOH, Hyeonjin ; CHOI, Eun-Mi ; KIM, Heon-Jung ; LEE, Sung-Ik ; YAMAMOTO, Tatsuharu ; KAWAE, Tatsuya ; TAKEDA, Kazuyoshi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-j403t-fa74856fa5781a3b27906361dc6d6ccdacd4e87ddf25b9aeac35d218b21a82d13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2001</creationdate><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Exact sciences and technology</topic><topic>Magnetic properties</topic><topic>Magnetic properties and materials</topic><topic>Metals, alloys and compounds (a15, 001c15, laves phases, chevrel phases, borocarbides, etc.)</topic><topic>Physics</topic><topic>Properties of type I and type II superconductors</topic><topic>Spin arrangements in magnetically ordered materials (including neutron and spin-polarized electron studies, synchrotron-source x-ray scattering, etc.)</topic><topic>Superconducting materials (excluding high-tc compounds)</topic><topic>Superconductivity</topic><topic>Ternary, quaternary and multinary compounds (including Chevrel phases, borocarbides etc.)</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>CHOI, Jae-Hyuk</creatorcontrib><creatorcontrib>DOH, Hyeonjin</creatorcontrib><creatorcontrib>CHOI, Eun-Mi</creatorcontrib><creatorcontrib>KIM, Heon-Jung</creatorcontrib><creatorcontrib>LEE, Sung-Ik</creatorcontrib><creatorcontrib>YAMAMOTO, Tatsuharu</creatorcontrib><creatorcontrib>KAWAE, Tatsuya</creatorcontrib><creatorcontrib>TAKEDA, Kazuyoshi</creatorcontrib><collection>Pascal-Francis</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of the Physical Society of Japan</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>CHOI, Jae-Hyuk</au><au>DOH, Hyeonjin</au><au>CHOI, Eun-Mi</au><au>KIM, Heon-Jung</au><au>LEE, Sung-Ik</au><au>YAMAMOTO, Tatsuharu</au><au>KAWAE, Tatsuya</au><au>TAKEDA, Kazuyoshi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Specific heat of field-dependent magnetic orderings in HoNi2B2C</atitle><jtitle>Journal of the Physical Society of Japan</jtitle><date>2001-10-01</date><risdate>2001</risdate><volume>70</volume><issue>10</issue><spage>3037</spage><epage>3041</epage><pages>3037-3041</pages><issn>0031-9015</issn><eissn>1347-4073</eissn><coden>JUPSAU</coden><abstract>We have investigated the low-temperature specific heat of HoNi2B2C down to T = 1 K in various magnetic fields from 0 T to 5 T. At zero field, the specific heat exhibits a large peak at TN = 5.1 K, which is due to commensurate antiferromagnetic ordering, and other smaller peak at T1 = 5.5 K, which is related to incommensurate ordering. As the field is increased up to 0.5 T, the first peak broadens and moves to a lower temperature, while the other peak at T1 moves to a higher temperature, which indicates that the phase between TN and T1 is more favored in magnetic fields. Among possible candidates for the phase, the a-axis modulation phase, which is an extension of a low temperature metamagnetic state, is the most probable. In the high-field region above 1 T, the two-peak feature is replaced by a broad-hill one that fades away with increasing fields, which is the typical smearing feature of the magnetic order at high fields.</abstract><cop>Tokyo</cop><pub>Institute of Pure and Applied Physics</pub><doi>10.1143/JPSJ.70.3037</doi><tpages>5</tpages></addata></record> |
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subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Exact sciences and technology Magnetic properties Magnetic properties and materials Metals, alloys and compounds (a15, 001c15, laves phases, chevrel phases, borocarbides, etc.) Physics Properties of type I and type II superconductors Spin arrangements in magnetically ordered materials (including neutron and spin-polarized electron studies, synchrotron-source x-ray scattering, etc.) Superconducting materials (excluding high-tc compounds) Superconductivity Ternary, quaternary and multinary compounds (including Chevrel phases, borocarbides etc.) |
title | Specific heat of field-dependent magnetic orderings in HoNi2B2C |
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