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Magnetic structures of R2RhSi3 (R=Ho, Er) compounds
Powder X-ray and neutron diffraction and magnetic measurements have been performed on R2RhSi3 (R=Ho and Er) compounds at low temperatures. The compounds crystallize in a derivative of the hexagonal AlB2-type structure. The crystal structure parameters have been refined on the basis of the X-ray and...
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Published in: | Journal of alloys and compounds 2003-10, Vol.360 (1-2), p.76-80 |
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container_title | Journal of alloys and compounds |
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creator | BAZELA, W WAWRZYNSKA, E PENC, B STÜSSER, N SZYTUŁA, A ZYGMUNT, A |
description | Powder X-ray and neutron diffraction and magnetic measurements have been performed on R2RhSi3 (R=Ho and Er) compounds at low temperatures. The compounds crystallize in a derivative of the hexagonal AlB2-type structure. The crystal structure parameters have been refined on the basis of the X-ray and neutron diffraction patterns collected in the paramagnetic region. These compounds are antiferromagnets with Neel temperatures of 5.2 K for Ho2RhSi3 and 5 K for Er2RhSi3. Both compounds exhibit collinear magnetic structures, described by the propagation vector k = (1 /2,0,0) for Ho2RhSi3 and k = (0,0,0) for Er2RhSi3. This magnetic order is stable in the temperature range between 1.5 K and the Neel temperature. |
doi_str_mv | 10.1016/S0925-8388(03)00374-8 |
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The compounds crystallize in a derivative of the hexagonal AlB2-type structure. The crystal structure parameters have been refined on the basis of the X-ray and neutron diffraction patterns collected in the paramagnetic region. These compounds are antiferromagnets with Neel temperatures of 5.2 K for Ho2RhSi3 and 5 K for Er2RhSi3. Both compounds exhibit collinear magnetic structures, described by the propagation vector k = (1 /2,0,0) for Ho2RhSi3 and k = (0,0,0) for Er2RhSi3. 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The compounds crystallize in a derivative of the hexagonal AlB2-type structure. The crystal structure parameters have been refined on the basis of the X-ray and neutron diffraction patterns collected in the paramagnetic region. These compounds are antiferromagnets with Neel temperatures of 5.2 K for Ho2RhSi3 and 5 K for Er2RhSi3. Both compounds exhibit collinear magnetic structures, described by the propagation vector k = (1 /2,0,0) for Ho2RhSi3 and k = (0,0,0) for Er2RhSi3. This magnetic order is stable in the temperature range between 1.5 K and the Neel temperature.</description><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Domain effects, magnetization curves, and hysteresis</subject><subject>Exact sciences and technology</subject><subject>Inorganic compounds</subject><subject>Magnetic properties and materials</subject><subject>Magnetization curves, hysteresis, Barkhausen and related effects</subject><subject>Magnetization curves, magnetization reversal, hysteresis, barkhausen and related effects</subject><subject>Physics</subject><subject>Structure of solids and liquids; crystallography</subject><subject>Structure of specific crystalline solids</subject><issn>0925-8388</issn><issn>1873-4669</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2003</creationdate><recordtype>article</recordtype><recordid>eNpFkE1Lw0AQhhdRsFZ_gpCL0oLR3Uw2u3vwIKVaoSK0el42k4lG0qTuJgf_vf1CYWAYeGaG92HsUvBbwUV2t-QmkbEGrUccxpyDSmN9xAZCK4jTLDPHbPCHnLKzEL4458KAGDB4cR8NdRVGofM9dr2nELVltEgWn8sKotHiftbeRFM_jrBdrdu-KcI5OyldHeji0Ifs_XH6NpnF89en58nDPEYQSRejzFNCnfPSKMjQEVECmciloZwKdCbX21LkFEqjCl2gEYR5jqlziTQwZNf7u2vffvcUOruqAlJdu4baPthEaQmawwaUexB9G4Kn0q59tXL-xwput4rsTpHd5rcc7E7RZhqyq8MDF9DVpXcNVuF_WSbAU5nCL8EtZe4</recordid><startdate>20031006</startdate><enddate>20031006</enddate><creator>BAZELA, W</creator><creator>WAWRZYNSKA, E</creator><creator>PENC, B</creator><creator>STÜSSER, N</creator><creator>SZYTUŁA, A</creator><creator>ZYGMUNT, A</creator><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20031006</creationdate><title>Magnetic structures of R2RhSi3 (R=Ho, Er) compounds</title><author>BAZELA, W ; WAWRZYNSKA, E ; PENC, B ; STÜSSER, N ; SZYTUŁA, A ; ZYGMUNT, A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c312t-c5b4ec8b0f9736caeee2361b59ebedca9b89b897ea7c597d8dc91ecbbc4aa2593</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Domain effects, magnetization curves, and hysteresis</topic><topic>Exact sciences and technology</topic><topic>Inorganic compounds</topic><topic>Magnetic properties and materials</topic><topic>Magnetization curves, hysteresis, Barkhausen and related effects</topic><topic>Magnetization curves, magnetization reversal, hysteresis, barkhausen and related effects</topic><topic>Physics</topic><topic>Structure of solids and liquids; crystallography</topic><topic>Structure of specific crystalline solids</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>BAZELA, W</creatorcontrib><creatorcontrib>WAWRZYNSKA, E</creatorcontrib><creatorcontrib>PENC, B</creatorcontrib><creatorcontrib>STÜSSER, N</creatorcontrib><creatorcontrib>SZYTUŁA, A</creatorcontrib><creatorcontrib>ZYGMUNT, A</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of alloys and compounds</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>BAZELA, W</au><au>WAWRZYNSKA, E</au><au>PENC, B</au><au>STÜSSER, N</au><au>SZYTUŁA, A</au><au>ZYGMUNT, A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Magnetic structures of R2RhSi3 (R=Ho, Er) compounds</atitle><jtitle>Journal of alloys and compounds</jtitle><date>2003-10-06</date><risdate>2003</risdate><volume>360</volume><issue>1-2</issue><spage>76</spage><epage>80</epage><pages>76-80</pages><issn>0925-8388</issn><eissn>1873-4669</eissn><abstract>Powder X-ray and neutron diffraction and magnetic measurements have been performed on R2RhSi3 (R=Ho and Er) compounds at low temperatures. The compounds crystallize in a derivative of the hexagonal AlB2-type structure. The crystal structure parameters have been refined on the basis of the X-ray and neutron diffraction patterns collected in the paramagnetic region. These compounds are antiferromagnets with Neel temperatures of 5.2 K for Ho2RhSi3 and 5 K for Er2RhSi3. Both compounds exhibit collinear magnetic structures, described by the propagation vector k = (1 /2,0,0) for Ho2RhSi3 and k = (0,0,0) for Er2RhSi3. This magnetic order is stable in the temperature range between 1.5 K and the Neel temperature.</abstract><cop>Lausanne</cop><pub>Elsevier</pub><doi>10.1016/S0925-8388(03)00374-8</doi><tpages>5</tpages></addata></record> |
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subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Condensed matter: structure, mechanical and thermal properties Domain effects, magnetization curves, and hysteresis Exact sciences and technology Inorganic compounds Magnetic properties and materials Magnetization curves, hysteresis, Barkhausen and related effects Magnetization curves, magnetization reversal, hysteresis, barkhausen and related effects Physics Structure of solids and liquids crystallography Structure of specific crystalline solids |
title | Magnetic structures of R2RhSi3 (R=Ho, Er) compounds |
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