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Synthesis, Characterization, and Magnetic Properties of New Rh(III) Compounds with the K4CdCl6Structure-Type:Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb)
The compounds Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb) have been synthesized and structurally characterized by Rietveld refinement of powder X-ray diffraction data in the space groupR3c;Z=6. The lattice parameters for the series were found to bea=9.78570(7) andc=11.4811(1) Å,a=9.7837(1) andc=11.44...
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Published in: | Journal of solid state chemistry 1998-08, Vol.139 (1), p.79-84 |
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description | The compounds Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb) have been synthesized and structurally characterized by Rietveld refinement of powder X-ray diffraction data in the space groupR3c;Z=6. The lattice parameters for the series were found to bea=9.78570(7) andc=11.4811(1) Å,a=9.7837(1) andc=11.4421(2) Å,a=9.7662(2) andc=11.3812(4) Å,a=9.7627(2) andc=11.3451(2) Å,a=9.7591(2) andc=11.3159(2) Å,a=9.7557(2) andc=11.2919(3) Å, anda=9.7390(2) andc=11.2501(3) Å, for Sr3SmRhO6, Sr3EuRhO6, Sr3TbRhO6, Sr3DyRhO6, Sr3HoRhO6, Sr3ErRhO6, and Sr3YbRhO6, respectively. These compounds are isostructural with K4CdCl6. The structure consists of infinite one-dimensional chains of alternating face-shared RhO6octahedra andMO6trigonal prisms (M=Sm, Eu, Tb, Dy, Ho, Er, and Yb). The strontium cations are located in a distorted square antiprismatic environment. Magnetic susceptibility data for the compounds Sr3MRhO6(M=Tb, Dy, Ho, Er, and Yb) obey the Curie law, with the expectedμeffvalues consistent with an oxidation state of +3 for both Rh andM. |
doi_str_mv | 10.1006/jssc.1998.7809 |
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The lattice parameters for the series were found to bea=9.78570(7) andc=11.4811(1) Å,a=9.7837(1) andc=11.4421(2) Å,a=9.7662(2) andc=11.3812(4) Å,a=9.7627(2) andc=11.3451(2) Å,a=9.7591(2) andc=11.3159(2) Å,a=9.7557(2) andc=11.2919(3) Å, anda=9.7390(2) andc=11.2501(3) Å, for Sr3SmRhO6, Sr3EuRhO6, Sr3TbRhO6, Sr3DyRhO6, Sr3HoRhO6, Sr3ErRhO6, and Sr3YbRhO6, respectively. These compounds are isostructural with K4CdCl6. The structure consists of infinite one-dimensional chains of alternating face-shared RhO6octahedra andMO6trigonal prisms (M=Sm, Eu, Tb, Dy, Ho, Er, and Yb). The strontium cations are located in a distorted square antiprismatic environment. Magnetic susceptibility data for the compounds Sr3MRhO6(M=Tb, Dy, Ho, Er, and Yb) obey the Curie law, with the expectedμeffvalues consistent with an oxidation state of +3 for both Rh andM.</description><identifier>ISSN: 0022-4596</identifier><identifier>EISSN: 1095-726X</identifier><identifier>DOI: 10.1006/jssc.1998.7809</identifier><language>eng</language><publisher>Elsevier Inc</publisher><subject>magnetic properties ; oxides ; rhodium(III) ; Rietveld refinement ; Sr3DyRhO6 ; Sr3ErRhO6 ; Sr3EuRhO6 ; Sr3HoRhO6 ; Sr3SmRhO6 ; Sr3TbRhO6 ; Sr3YbRhO6</subject><ispartof>Journal of solid state chemistry, 1998-08, Vol.139 (1), p.79-84</ispartof><rights>1998 Academic Press</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c201t-6dc4876f217acfe224b59291e069c7788c6b317426f72156992bd086ac4047223</citedby><cites>FETCH-LOGICAL-c201t-6dc4876f217acfe224b59291e069c7788c6b317426f72156992bd086ac4047223</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Layland, Ralph C</creatorcontrib><creatorcontrib>Kirkland, Shalawn L</creatorcontrib><creatorcontrib>zur Loye, Hans-Conrad</creatorcontrib><title>Synthesis, Characterization, and Magnetic Properties of New Rh(III) Compounds with the K4CdCl6Structure-Type:Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb)</title><title>Journal of solid state chemistry</title><description>The compounds Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb) have been synthesized and structurally characterized by Rietveld refinement of powder X-ray diffraction data in the space groupR3c;Z=6. The lattice parameters for the series were found to bea=9.78570(7) andc=11.4811(1) Å,a=9.7837(1) andc=11.4421(2) Å,a=9.7662(2) andc=11.3812(4) Å,a=9.7627(2) andc=11.3451(2) Å,a=9.7591(2) andc=11.3159(2) Å,a=9.7557(2) andc=11.2919(3) Å, anda=9.7390(2) andc=11.2501(3) Å, for Sr3SmRhO6, Sr3EuRhO6, Sr3TbRhO6, Sr3DyRhO6, Sr3HoRhO6, Sr3ErRhO6, and Sr3YbRhO6, respectively. These compounds are isostructural with K4CdCl6. The structure consists of infinite one-dimensional chains of alternating face-shared RhO6octahedra andMO6trigonal prisms (M=Sm, Eu, Tb, Dy, Ho, Er, and Yb). The strontium cations are located in a distorted square antiprismatic environment. Magnetic susceptibility data for the compounds Sr3MRhO6(M=Tb, Dy, Ho, Er, and Yb) obey the Curie law, with the expectedμeffvalues consistent with an oxidation state of +3 for both Rh andM.</description><subject>magnetic properties</subject><subject>oxides</subject><subject>rhodium(III)</subject><subject>Rietveld refinement</subject><subject>Sr3DyRhO6</subject><subject>Sr3ErRhO6</subject><subject>Sr3EuRhO6</subject><subject>Sr3HoRhO6</subject><subject>Sr3SmRhO6</subject><subject>Sr3TbRhO6</subject><subject>Sr3YbRhO6</subject><issn>0022-4596</issn><issn>1095-726X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1998</creationdate><recordtype>article</recordtype><recordid>eNp1kM9LwzAYhoMoOH9cPeeo0M4ka5NG8CB1uuLmxE3QU0nTrzaytSPJlPqP-O-6Ma-ePt7D874fD0JnlPQpIfzywzndp1ImfZEQuYd6lMg4FIy_7qMeIYyFUSz5ITpy7oMQSuMk6qGfWdf4GpxxAU5rZZX2YM238qZtAqyaEk_UewPeaPxk2xVYb8DhtsKP8IWf6_Msyy5w2i5X7bopHf4yvsabPvwQpWW64DNv19qvLYTzbgVXMzuYPNdTfj65ni0DPFwHeF4E-LYL8KjdZLubfCsuTtBBpRYOTv_uMXq5G87TUTie3mfpzTjUjFAf8lJHieAVo0LpChiLilgySYFwqYVIEs2LARUR45VgNOZSsqIkCVc6IpFgbHCM-rtebVvnLFT5ypqlsl1OSb7Vmm-15lut-VbrBkh2AGy--jRgc6cNNBpKY0H7vGzNf-gvPSR8AQ</recordid><startdate>199808</startdate><enddate>199808</enddate><creator>Layland, Ralph C</creator><creator>Kirkland, Shalawn L</creator><creator>zur Loye, Hans-Conrad</creator><general>Elsevier Inc</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>199808</creationdate><title>Synthesis, Characterization, and Magnetic Properties of New Rh(III) Compounds with the K4CdCl6Structure-Type:Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb)</title><author>Layland, Ralph C ; Kirkland, Shalawn L ; zur Loye, Hans-Conrad</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c201t-6dc4876f217acfe224b59291e069c7788c6b317426f72156992bd086ac4047223</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1998</creationdate><topic>magnetic properties</topic><topic>oxides</topic><topic>rhodium(III)</topic><topic>Rietveld refinement</topic><topic>Sr3DyRhO6</topic><topic>Sr3ErRhO6</topic><topic>Sr3EuRhO6</topic><topic>Sr3HoRhO6</topic><topic>Sr3SmRhO6</topic><topic>Sr3TbRhO6</topic><topic>Sr3YbRhO6</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Layland, Ralph C</creatorcontrib><creatorcontrib>Kirkland, Shalawn L</creatorcontrib><creatorcontrib>zur Loye, Hans-Conrad</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of solid state chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Layland, Ralph C</au><au>Kirkland, Shalawn L</au><au>zur Loye, Hans-Conrad</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Synthesis, Characterization, and Magnetic Properties of New Rh(III) Compounds with the K4CdCl6Structure-Type:Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb)</atitle><jtitle>Journal of solid state chemistry</jtitle><date>1998-08</date><risdate>1998</risdate><volume>139</volume><issue>1</issue><spage>79</spage><epage>84</epage><pages>79-84</pages><issn>0022-4596</issn><eissn>1095-726X</eissn><abstract>The compounds Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb) have been synthesized and structurally characterized by Rietveld refinement of powder X-ray diffraction data in the space groupR3c;Z=6. The lattice parameters for the series were found to bea=9.78570(7) andc=11.4811(1) Å,a=9.7837(1) andc=11.4421(2) Å,a=9.7662(2) andc=11.3812(4) Å,a=9.7627(2) andc=11.3451(2) Å,a=9.7591(2) andc=11.3159(2) Å,a=9.7557(2) andc=11.2919(3) Å, anda=9.7390(2) andc=11.2501(3) Å, for Sr3SmRhO6, Sr3EuRhO6, Sr3TbRhO6, Sr3DyRhO6, Sr3HoRhO6, Sr3ErRhO6, and Sr3YbRhO6, respectively. These compounds are isostructural with K4CdCl6. The structure consists of infinite one-dimensional chains of alternating face-shared RhO6octahedra andMO6trigonal prisms (M=Sm, Eu, Tb, Dy, Ho, Er, and Yb). The strontium cations are located in a distorted square antiprismatic environment. Magnetic susceptibility data for the compounds Sr3MRhO6(M=Tb, Dy, Ho, Er, and Yb) obey the Curie law, with the expectedμeffvalues consistent with an oxidation state of +3 for both Rh andM.</abstract><pub>Elsevier Inc</pub><doi>10.1006/jssc.1998.7809</doi><tpages>6</tpages></addata></record> |
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subjects | magnetic properties oxides rhodium(III) Rietveld refinement Sr3DyRhO6 Sr3ErRhO6 Sr3EuRhO6 Sr3HoRhO6 Sr3SmRhO6 Sr3TbRhO6 Sr3YbRhO6 |
title | Synthesis, Characterization, and Magnetic Properties of New Rh(III) Compounds with the K4CdCl6Structure-Type:Sr3MRhO6(M=Sm, Eu, Tb, Dy, Ho, Er, and Yb) |
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