1-D Polymers with Alternate Cu2 and Ln2 Units (Ln = Gd, Er, Y) and Carboxylate Linkages

Three isostructural Cu2Ln2 1-D polymers [Cu2Ln2L10(H2O)4·3H2O] n where Ln = Gd (1), Er (2), and Y (3) and HL= trans-2-butenoic acid, were synthesized and characterized by X-ray crystallography, electron paramagnetic resonance, and magnetic measurements. Pairs of alternate Cu2 and Ln2 dinuclear units...

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Veröffentlicht in:Inorganic chemistry 2008-11, Vol.47 (22), p.10389-10397
Hauptverfasser: Calvo, Rafael, Rapp, Raul E, Chagas, Edson, Sartoris, Rosana P, Baggio, Ricardo, Garland, María T, Perec, Mireille
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container_end_page 10397
container_issue 22
container_start_page 10389
container_title Inorganic chemistry
container_volume 47
creator Calvo, Rafael
Rapp, Raul E
Chagas, Edson
Sartoris, Rosana P
Baggio, Ricardo
Garland, María T
Perec, Mireille
description Three isostructural Cu2Ln2 1-D polymers [Cu2Ln2L10(H2O)4·3H2O] n where Ln = Gd (1), Er (2), and Y (3) and HL= trans-2-butenoic acid, were synthesized and characterized by X-ray crystallography, electron paramagnetic resonance, and magnetic measurements. Pairs of alternate Cu2 and Ln2 dinuclear units are combined into a linear array by a set of one covalent η2:η1:μ2 carboxylate oxygen and two H bonds, at Cu···Ln distances of ca. 4.5 Å. These units exhibit four η1:η1:μ2 and two η2:η1:μ2 carboxylate bridges, respectively. Magnetic measurements between 2 and 300 K, fields B 0 = μ0 H between 0 and 9 T, and electron paramagnetic resonance (EPR) measurements at the X-band and room temperature are reported. The magnetic susceptibilities indicate bulk antiferromagnetic behavior of the three compounds at low temperatures. Magnetization and EPR data for 1 and 3 allowed evaluation of the exchange couplings between both Cu and Gd ions in their dinuclear units and between Cu and Gd neighbor ions in the spin chains. The data for the isolated Cu2 units in 3 yield g || = 2.350 and g ⊥ = 2.054, J Cu−Cu = −338 (3) cm−1 for the exchange coupling [H ex(1,2) = −J 1−2 S 1·S 2], and D 0 = −0.342 (0.003) cm−1 and E 0 = 0.003 (0.001) cm−1 for the zero-field-splitting parameters of the triplet state arising from anisotropic spin−spin interactions. Considering tetranuclear blocks Gd−Cu−Cu−Gd in 1, with the parameters for the Cu2 unit obtained for 3, we evaluated ferromagnetic interactions between Cu and Gd neighbors, J Cu−Gd = 13.0 (0.1) cm−1, and between Gd ions in the Gd2 units, J Gd−Gd = 0.25 (0.02) cm−1, with g Gd = 1.991. The bulk antiferromagnetic behavior of 1 is a consequence of the antiferromagnetic coupling between Cu ions and of the magnitude, |J Cu−Gd|, of the Cu−Gd exchange coupling. Compound 2 displays a susceptibility peak at 15 K that may be interpreted as the combined result from antiferromagnetic couplings between ErIII ions in Er2 units and their coupling with the Cu2 units.
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Pairs of alternate Cu2 and Ln2 dinuclear units are combined into a linear array by a set of one covalent η2:η1:μ2 carboxylate oxygen and two H bonds, at Cu···Ln distances of ca. 4.5 Å. These units exhibit four η1:η1:μ2 and two η2:η1:μ2 carboxylate bridges, respectively. Magnetic measurements between 2 and 300 K, fields B 0 = μ0 H between 0 and 9 T, and electron paramagnetic resonance (EPR) measurements at the X-band and room temperature are reported. The magnetic susceptibilities indicate bulk antiferromagnetic behavior of the three compounds at low temperatures. Magnetization and EPR data for 1 and 3 allowed evaluation of the exchange couplings between both Cu and Gd ions in their dinuclear units and between Cu and Gd neighbor ions in the spin chains. The data for the isolated Cu2 units in 3 yield g || = 2.350 and g ⊥ = 2.054, J Cu−Cu = −338 (3) cm−1 for the exchange coupling [H ex(1,2) = −J 1−2 S 1·S 2], and D 0 = −0.342 (0.003) cm−1 and E 0 = 0.003 (0.001) cm−1 for the zero-field-splitting parameters of the triplet state arising from anisotropic spin−spin interactions. Considering tetranuclear blocks Gd−Cu−Cu−Gd in 1, with the parameters for the Cu2 unit obtained for 3, we evaluated ferromagnetic interactions between Cu and Gd neighbors, J Cu−Gd = 13.0 (0.1) cm−1, and between Gd ions in the Gd2 units, J Gd−Gd = 0.25 (0.02) cm−1, with g Gd = 1.991. The bulk antiferromagnetic behavior of 1 is a consequence of the antiferromagnetic coupling between Cu ions and of the magnitude, |J Cu−Gd|, of the Cu−Gd exchange coupling. 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Chem</addtitle><description>Three isostructural Cu2Ln2 1-D polymers [Cu2Ln2L10(H2O)4·3H2O] n where Ln = Gd (1), Er (2), and Y (3) and HL= trans-2-butenoic acid, were synthesized and characterized by X-ray crystallography, electron paramagnetic resonance, and magnetic measurements. Pairs of alternate Cu2 and Ln2 dinuclear units are combined into a linear array by a set of one covalent η2:η1:μ2 carboxylate oxygen and two H bonds, at Cu···Ln distances of ca. 4.5 Å. These units exhibit four η1:η1:μ2 and two η2:η1:μ2 carboxylate bridges, respectively. Magnetic measurements between 2 and 300 K, fields B 0 = μ0 H between 0 and 9 T, and electron paramagnetic resonance (EPR) measurements at the X-band and room temperature are reported. The magnetic susceptibilities indicate bulk antiferromagnetic behavior of the three compounds at low temperatures. Magnetization and EPR data for 1 and 3 allowed evaluation of the exchange couplings between both Cu and Gd ions in their dinuclear units and between Cu and Gd neighbor ions in the spin chains. The data for the isolated Cu2 units in 3 yield g || = 2.350 and g ⊥ = 2.054, J Cu−Cu = −338 (3) cm−1 for the exchange coupling [H ex(1,2) = −J 1−2 S 1·S 2], and D 0 = −0.342 (0.003) cm−1 and E 0 = 0.003 (0.001) cm−1 for the zero-field-splitting parameters of the triplet state arising from anisotropic spin−spin interactions. Considering tetranuclear blocks Gd−Cu−Cu−Gd in 1, with the parameters for the Cu2 unit obtained for 3, we evaluated ferromagnetic interactions between Cu and Gd neighbors, J Cu−Gd = 13.0 (0.1) cm−1, and between Gd ions in the Gd2 units, J Gd−Gd = 0.25 (0.02) cm−1, with g Gd = 1.991. The bulk antiferromagnetic behavior of 1 is a consequence of the antiferromagnetic coupling between Cu ions and of the magnitude, |J Cu−Gd|, of the Cu−Gd exchange coupling. Compound 2 displays a susceptibility peak at 15 K that may be interpreted as the combined result from antiferromagnetic couplings between ErIII ions in Er2 units and their coupling with the Cu2 units.</description><subject>Copper - chemistry</subject><subject>Crotonates - chemistry</subject><subject>Crystallography, X-Ray</subject><subject>Electron Spin Resonance Spectroscopy</subject><subject>Hydrogen Bonding</subject><subject>Lanthanoid Series Elements - chemistry</subject><subject>Ligands</subject><subject>Magnetics</subject><subject>Models, Chemical</subject><subject>Models, Molecular</subject><subject>Organometallic Compounds - chemistry</subject><subject>Polymers - chemistry</subject><issn>0020-1669</issn><issn>1520-510X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNo9kUtPwzAQhC0EouVx4A8gX0AgEdi14yQ-cIDwViRAtKKcLCdxICUPiBNB_z2Blp5mpfl2DjOE7CAcIzA8yZMA0IVArpAhCgaOQJiskiFAf6PnyQHZsHYKAJK73joZYCC57woYkmd0LuhDXcxK01j6lbdv9KxoTVPp1tCwY1RXKY0qRsdV3lp6EFX0lF6nR_SyOaIvh392qJu4_p4Vvy9RXr3rV2O3yFqmC2u2F7pJxleXo_DGie6vb8OzyNHM91sn5gIE-NqTaRYL48og4AFI5Bl3hYmTmCdoMpbEGTIPBfKU-dpNuE4TCDA1fJPsz3M_mvqzM7ZVZW4TUxS6MnVnlSd9IT0MenB3AXZxaVL10eSlbmbqv4oecOZAblvzvfR18648n_tCjR6e1M15yCaPd1cKe35vzuvEqmnd9ZUVViGo30nUchL-A7YndpQ</recordid><startdate>20081117</startdate><enddate>20081117</enddate><creator>Calvo, Rafael</creator><creator>Rapp, Raul E</creator><creator>Chagas, Edson</creator><creator>Sartoris, Rosana P</creator><creator>Baggio, Ricardo</creator><creator>Garland, María T</creator><creator>Perec, Mireille</creator><general>American Chemical Society</general><scope>BSCLL</scope><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>7X8</scope></search><sort><creationdate>20081117</creationdate><title>1-D Polymers with Alternate Cu2 and Ln2 Units (Ln = Gd, Er, Y) and Carboxylate Linkages</title><author>Calvo, Rafael ; Rapp, Raul E ; Chagas, Edson ; Sartoris, Rosana P ; Baggio, Ricardo ; Garland, María T ; Perec, Mireille</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a277t-b350507a69dfb5e4988380913f345ebcb3c1ef2cbf1261513d27a4c3adc081de3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>Copper - chemistry</topic><topic>Crotonates - chemistry</topic><topic>Crystallography, X-Ray</topic><topic>Electron Spin Resonance Spectroscopy</topic><topic>Hydrogen Bonding</topic><topic>Lanthanoid Series Elements - chemistry</topic><topic>Ligands</topic><topic>Magnetics</topic><topic>Models, Chemical</topic><topic>Models, Molecular</topic><topic>Organometallic Compounds - chemistry</topic><topic>Polymers - chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Calvo, Rafael</creatorcontrib><creatorcontrib>Rapp, Raul E</creatorcontrib><creatorcontrib>Chagas, Edson</creatorcontrib><creatorcontrib>Sartoris, Rosana P</creatorcontrib><creatorcontrib>Baggio, Ricardo</creatorcontrib><creatorcontrib>Garland, María T</creatorcontrib><creatorcontrib>Perec, Mireille</creatorcontrib><collection>Istex</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>Inorganic chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Calvo, Rafael</au><au>Rapp, Raul E</au><au>Chagas, Edson</au><au>Sartoris, Rosana P</au><au>Baggio, Ricardo</au><au>Garland, María T</au><au>Perec, Mireille</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>1-D Polymers with Alternate Cu2 and Ln2 Units (Ln = Gd, Er, Y) and Carboxylate Linkages</atitle><jtitle>Inorganic chemistry</jtitle><addtitle>Inorg. Chem</addtitle><date>2008-11-17</date><risdate>2008</risdate><volume>47</volume><issue>22</issue><spage>10389</spage><epage>10397</epage><pages>10389-10397</pages><issn>0020-1669</issn><eissn>1520-510X</eissn><abstract>Three isostructural Cu2Ln2 1-D polymers [Cu2Ln2L10(H2O)4·3H2O] n where Ln = Gd (1), Er (2), and Y (3) and HL= trans-2-butenoic acid, were synthesized and characterized by X-ray crystallography, electron paramagnetic resonance, and magnetic measurements. Pairs of alternate Cu2 and Ln2 dinuclear units are combined into a linear array by a set of one covalent η2:η1:μ2 carboxylate oxygen and two H bonds, at Cu···Ln distances of ca. 4.5 Å. These units exhibit four η1:η1:μ2 and two η2:η1:μ2 carboxylate bridges, respectively. Magnetic measurements between 2 and 300 K, fields B 0 = μ0 H between 0 and 9 T, and electron paramagnetic resonance (EPR) measurements at the X-band and room temperature are reported. The magnetic susceptibilities indicate bulk antiferromagnetic behavior of the three compounds at low temperatures. Magnetization and EPR data for 1 and 3 allowed evaluation of the exchange couplings between both Cu and Gd ions in their dinuclear units and between Cu and Gd neighbor ions in the spin chains. The data for the isolated Cu2 units in 3 yield g || = 2.350 and g ⊥ = 2.054, J Cu−Cu = −338 (3) cm−1 for the exchange coupling [H ex(1,2) = −J 1−2 S 1·S 2], and D 0 = −0.342 (0.003) cm−1 and E 0 = 0.003 (0.001) cm−1 for the zero-field-splitting parameters of the triplet state arising from anisotropic spin−spin interactions. Considering tetranuclear blocks Gd−Cu−Cu−Gd in 1, with the parameters for the Cu2 unit obtained for 3, we evaluated ferromagnetic interactions between Cu and Gd neighbors, J Cu−Gd = 13.0 (0.1) cm−1, and between Gd ions in the Gd2 units, J Gd−Gd = 0.25 (0.02) cm−1, with g Gd = 1.991. The bulk antiferromagnetic behavior of 1 is a consequence of the antiferromagnetic coupling between Cu ions and of the magnitude, |J Cu−Gd|, of the Cu−Gd exchange coupling. Compound 2 displays a susceptibility peak at 15 K that may be interpreted as the combined result from antiferromagnetic couplings between ErIII ions in Er2 units and their coupling with the Cu2 units.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>18937450</pmid><doi>10.1021/ic8014089</doi><tpages>9</tpages><oa>free_for_read</oa></addata></record>
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subjects Copper - chemistry
Crotonates - chemistry
Crystallography, X-Ray
Electron Spin Resonance Spectroscopy
Hydrogen Bonding
Lanthanoid Series Elements - chemistry
Ligands
Magnetics
Models, Chemical
Models, Molecular
Organometallic Compounds - chemistry
Polymers - chemistry
title 1-D Polymers with Alternate Cu2 and Ln2 Units (Ln = Gd, Er, Y) and Carboxylate Linkages
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