Ferromagnetic Coupling in a 1D Coordination Polymer Containing a Symmetric [Cu(μ1,1-N3)2Cu(μ1,1-N3)2Cu]2+ Core and Based on an Organic Ligand Obtained from the Solid State

Addition of rctt-tetrakis(2-pyridyl)cyclobutane (2,2‘-tpcb) in a CuII/N3 - solution afforded the 1D coordination polymer [Cu3(N3)6(2,2‘-tpcb)(DMF)2] n (1). The ligand 2,2‘-tpcb serves as a tetradentate bis-chelating ligand by linking linear [(DMF)Cu(μ1,1-N3)2Cu(N3)2(μ1,1-N3)2Cu(DMF)] trinuclear unit...

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Veröffentlicht in:Inorganic chemistry 2007-10, Vol.46 (21), p.8843-8850
Hauptverfasser: Stamatatos, Theocharis C, Papaefstathiou, Giannis S, MacGillivray, Leonard R, Escuer, Albert, Vicente, Ramon, Ruiz, Eliseo, Perlepes, Spyros P
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container_end_page 8850
container_issue 21
container_start_page 8843
container_title Inorganic chemistry
container_volume 46
creator Stamatatos, Theocharis C
Papaefstathiou, Giannis S
MacGillivray, Leonard R
Escuer, Albert
Vicente, Ramon
Ruiz, Eliseo
Perlepes, Spyros P
description Addition of rctt-tetrakis(2-pyridyl)cyclobutane (2,2‘-tpcb) in a CuII/N3 - solution afforded the 1D coordination polymer [Cu3(N3)6(2,2‘-tpcb)(DMF)2] n (1). The ligand 2,2‘-tpcb serves as a tetradentate bis-chelating ligand by linking linear [(DMF)Cu(μ1,1-N3)2Cu(N3)2(μ1,1-N3)2Cu(DMF)] trinuclear units to produce a zigzag chain. Within each centrosymmetric trinuclear unit there exist two irregularly asymmetric end-on double azido-bridged [Cu(μ1,1-N3)2Cu]2+ cores, while one of the largest Cu−Nazide−Cu angles is observed. Magnetic susceptibility data, measured from 2 to 300 K, show bulk moderate ferromagnetic coupling within the magnetically isolated trinuclear units. These data were fitted to the appropriate equation derived from the Hamiltonian H = −J 1(S A1 S B + S A2 S B) − J 2 S A1 S A2, giving the parameters J 1 = +70(3) cm-1, J 2 = −3(2) cm-1, g = 2.12(1), with an intertrimer interaction parameter θ = −0.74(2) K. The coupling constants were correlated with the structural parameters. Density functional calculations reproduce very well the experimental J values and show that ferromagnetism for this complex is mainly due to the topology of the magnetic orbitals and the different coordination spheres of two neighboring CuII atoms, resulting in a small overlap of the orbitals possessing the unpaired electrons.
doi_str_mv 10.1021/ic070018b
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The ligand 2,2‘-tpcb serves as a tetradentate bis-chelating ligand by linking linear [(DMF)Cu(μ1,1-N3)2Cu(N3)2(μ1,1-N3)2Cu(DMF)] trinuclear units to produce a zigzag chain. Within each centrosymmetric trinuclear unit there exist two irregularly asymmetric end-on double azido-bridged [Cu(μ1,1-N3)2Cu]2+ cores, while one of the largest Cu−Nazide−Cu angles is observed. Magnetic susceptibility data, measured from 2 to 300 K, show bulk moderate ferromagnetic coupling within the magnetically isolated trinuclear units. These data were fitted to the appropriate equation derived from the Hamiltonian H = −J 1(S A1 S B + S A2 S B) − J 2 S A1 S A2, giving the parameters J 1 = +70(3) cm-1, J 2 = −3(2) cm-1, g = 2.12(1), with an intertrimer interaction parameter θ = −0.74(2) K. The coupling constants were correlated with the structural parameters. 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Chem</addtitle><description>Addition of rctt-tetrakis(2-pyridyl)cyclobutane (2,2‘-tpcb) in a CuII/N3 - solution afforded the 1D coordination polymer [Cu3(N3)6(2,2‘-tpcb)(DMF)2] n (1). The ligand 2,2‘-tpcb serves as a tetradentate bis-chelating ligand by linking linear [(DMF)Cu(μ1,1-N3)2Cu(N3)2(μ1,1-N3)2Cu(DMF)] trinuclear units to produce a zigzag chain. Within each centrosymmetric trinuclear unit there exist two irregularly asymmetric end-on double azido-bridged [Cu(μ1,1-N3)2Cu]2+ cores, while one of the largest Cu−Nazide−Cu angles is observed. Magnetic susceptibility data, measured from 2 to 300 K, show bulk moderate ferromagnetic coupling within the magnetically isolated trinuclear units. These data were fitted to the appropriate equation derived from the Hamiltonian H = −J 1(S A1 S B + S A2 S B) − J 2 S A1 S A2, giving the parameters J 1 = +70(3) cm-1, J 2 = −3(2) cm-1, g = 2.12(1), with an intertrimer interaction parameter θ = −0.74(2) K. 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These data were fitted to the appropriate equation derived from the Hamiltonian H = −J 1(S A1 S B + S A2 S B) − J 2 S A1 S A2, giving the parameters J 1 = +70(3) cm-1, J 2 = −3(2) cm-1, g = 2.12(1), with an intertrimer interaction parameter θ = −0.74(2) K. The coupling constants were correlated with the structural parameters. Density functional calculations reproduce very well the experimental J values and show that ferromagnetism for this complex is mainly due to the topology of the magnetic orbitals and the different coordination spheres of two neighboring CuII atoms, resulting in a small overlap of the orbitals possessing the unpaired electrons.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>17867673</pmid><doi>10.1021/ic070018b</doi><tpages>8</tpages></addata></record>
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title Ferromagnetic Coupling in a 1D Coordination Polymer Containing a Symmetric [Cu(μ1,1-N3)2Cu(μ1,1-N3)2Cu]2+ Core and Based on an Organic Ligand Obtained from the Solid State
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