Crystallographic, magnetic and electrical characteristics of R^sub 3^Ni^sub 8^Sn^sub 4^ compounds (R = Y, Nd, Sm, Gd, and Tb)
The R3Ni8Sn4 compounds (R = Y, Nd, Sm, Gd, and Tb) have been synthesized and studied by powder X-ray diffraction, magnetic and electrical properties measurements. They crystallize in Lu3Co7.77Sn4 structure type (space group P63mc), and are characterized by different occupancy of some atomic position...
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creator | Romaka, VV Romaka, L Romaniv, I Hlil, EK Rykavets, Z Kuzhel, B |
description | The R3Ni8Sn4 compounds (R = Y, Nd, Sm, Gd, and Tb) have been synthesized and studied by powder X-ray diffraction, magnetic and electrical properties measurements. They crystallize in Lu3Co7.77Sn4 structure type (space group P63mc), and are characterized by different occupancy of some atomic positions, giving 3:8:4 stoichiometry in one case or statistical mixture of Ni and Sn in the other. The magnetic properties were studied in the temperature range 2-300 K and showed that at low temperatures Gd3Ni8Sn4 and Tb3Ni8Sn4 compounds exhibit ferromagnetic and antiferromagnetic ordering, respectively, while at higher temperatures both stannides are Curie-Weiss paramagnets. The Y3Ni8Sn4 stannide is a Pauli paramagnet while in Sm3Ni8Sn4 the magnetism is weak in the temperature range 2-300 K. The electrical properties of the R3Ni8Sn4 compounds showed metallic type of conductivity. The performed electronic structure calculations of Y3Ni8Sn4 are in a good agreement with electrical and magnetic studies. |
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They crystallize in Lu3Co7.77Sn4 structure type (space group P63mc), and are characterized by different occupancy of some atomic positions, giving 3:8:4 stoichiometry in one case or statistical mixture of Ni and Sn in the other. The magnetic properties were studied in the temperature range 2-300 K and showed that at low temperatures Gd3Ni8Sn4 and Tb3Ni8Sn4 compounds exhibit ferromagnetic and antiferromagnetic ordering, respectively, while at higher temperatures both stannides are Curie-Weiss paramagnets. The Y3Ni8Sn4 stannide is a Pauli paramagnet while in Sm3Ni8Sn4 the magnetism is weak in the temperature range 2-300 K. The electrical properties of the R3Ni8Sn4 compounds showed metallic type of conductivity. 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They crystallize in Lu3Co7.77Sn4 structure type (space group P63mc), and are characterized by different occupancy of some atomic positions, giving 3:8:4 stoichiometry in one case or statistical mixture of Ni and Sn in the other. The magnetic properties were studied in the temperature range 2-300 K and showed that at low temperatures Gd3Ni8Sn4 and Tb3Ni8Sn4 compounds exhibit ferromagnetic and antiferromagnetic ordering, respectively, while at higher temperatures both stannides are Curie-Weiss paramagnets. The Y3Ni8Sn4 stannide is a Pauli paramagnet while in Sm3Ni8Sn4 the magnetism is weak in the temperature range 2-300 K. The electrical properties of the R3Ni8Sn4 compounds showed metallic type of conductivity. The performed electronic structure calculations of Y3Ni8Sn4 are in a good agreement with electrical and magnetic studies.</description><subject>Antiferromagnetism</subject><subject>Atomic structure</subject><subject>Chemical compounds</subject><subject>Conductivity</subject><subject>Crystallization</subject><subject>Crystallography</subject><subject>Diffraction</subject><subject>Electrical properties</subject><subject>Electrical resistivity</subject><subject>Electronic structure</subject><subject>Ferromagnetism</subject><subject>Magnetic properties</subject><subject>Magnetism</subject><subject>Samarium compounds</subject><subject>Stannides</subject><subject>Temperature</subject><subject>Tin compounds</subject><issn>0925-8388</issn><issn>1873-4669</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNqNjrFuwjAURa2qSE1L_-FJXUBKJAeH1BmYEIWJAVhYEjmOASPHTv2coUP_nRTxAZ3ukc7V1X0iUco_WZLlefFMIlrM5glnnL-QV8QrpTQtWBqR36X_wSCMcWcvuouWMbTibFXQEoRtQBklg9dSGJAX4YUMymscLII7wa7EvgZWbvUdeLm3d8hKkK7tXG8bhMkOFnCMYdvEsG9jWA_5N32op2MyOgmD6v2Rb-Tja3VYbpLOu-9eYaiurvd2UNVwNyvmKaM5-1_rBiHtTZY</recordid><startdate>20170415</startdate><enddate>20170415</enddate><creator>Romaka, VV</creator><creator>Romaka, L</creator><creator>Romaniv, I</creator><creator>Hlil, EK</creator><creator>Rykavets, Z</creator><creator>Kuzhel, B</creator><general>Elsevier BV</general><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20170415</creationdate><title>Crystallographic, magnetic and electrical characteristics of R^sub 3^Ni^sub 8^Sn^sub 4^ compounds (R = Y, Nd, Sm, Gd, and Tb)</title><author>Romaka, VV ; Romaka, L ; Romaniv, I ; Hlil, EK ; Rykavets, Z ; Kuzhel, B</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_19349513063</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Antiferromagnetism</topic><topic>Atomic structure</topic><topic>Chemical compounds</topic><topic>Conductivity</topic><topic>Crystallization</topic><topic>Crystallography</topic><topic>Diffraction</topic><topic>Electrical properties</topic><topic>Electrical resistivity</topic><topic>Electronic structure</topic><topic>Ferromagnetism</topic><topic>Magnetic properties</topic><topic>Magnetism</topic><topic>Samarium compounds</topic><topic>Stannides</topic><topic>Temperature</topic><topic>Tin compounds</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Romaka, VV</creatorcontrib><creatorcontrib>Romaka, L</creatorcontrib><creatorcontrib>Romaniv, I</creatorcontrib><creatorcontrib>Hlil, EK</creatorcontrib><creatorcontrib>Rykavets, Z</creatorcontrib><creatorcontrib>Kuzhel, B</creatorcontrib><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>Romaka, VV</au><au>Romaka, L</au><au>Romaniv, I</au><au>Hlil, EK</au><au>Rykavets, Z</au><au>Kuzhel, B</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Crystallographic, magnetic and electrical characteristics of R^sub 3^Ni^sub 8^Sn^sub 4^ compounds (R = Y, Nd, Sm, Gd, and Tb)</atitle><jtitle>Journal of alloys and compounds</jtitle><date>2017-04-15</date><risdate>2017</risdate><volume>701</volume><spage>358</spage><pages>358-</pages><issn>0925-8388</issn><eissn>1873-4669</eissn><abstract>The R3Ni8Sn4 compounds (R = Y, Nd, Sm, Gd, and Tb) have been synthesized and studied by powder X-ray diffraction, magnetic and electrical properties measurements. They crystallize in Lu3Co7.77Sn4 structure type (space group P63mc), and are characterized by different occupancy of some atomic positions, giving 3:8:4 stoichiometry in one case or statistical mixture of Ni and Sn in the other. The magnetic properties were studied in the temperature range 2-300 K and showed that at low temperatures Gd3Ni8Sn4 and Tb3Ni8Sn4 compounds exhibit ferromagnetic and antiferromagnetic ordering, respectively, while at higher temperatures both stannides are Curie-Weiss paramagnets. The Y3Ni8Sn4 stannide is a Pauli paramagnet while in Sm3Ni8Sn4 the magnetism is weak in the temperature range 2-300 K. The electrical properties of the R3Ni8Sn4 compounds showed metallic type of conductivity. The performed electronic structure calculations of Y3Ni8Sn4 are in a good agreement with electrical and magnetic studies.</abstract><cop>Lausanne</cop><pub>Elsevier BV</pub></addata></record> |
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subjects | Antiferromagnetism Atomic structure Chemical compounds Conductivity Crystallization Crystallography Diffraction Electrical properties Electrical resistivity Electronic structure Ferromagnetism Magnetic properties Magnetism Samarium compounds Stannides Temperature Tin compounds |
title | Crystallographic, magnetic and electrical characteristics of R^sub 3^Ni^sub 8^Sn^sub 4^ compounds (R = Y, Nd, Sm, Gd, and Tb) |
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