Structural and Magnetic Properties of MnIII and CuII Tetranuclear Azido Polyoxometalate Complexes: Multifrequency High‐Field EPR Spectroscopy of Cu4 Clusters with S=1 and S=2 Ground States

作者: Pierre Mialane , Carole Duboc , Jérôme Marrot , Eric Rivière , Anne Dolbecq

DOI: 10.1002/CHEM.200500877

关键词: ParamagnetismCrystallographyChemistryExcited statePolyoxometalateAntiferromagnetismSpin statesMagnetic susceptibilityInorganic chemistryElectron paramagnetic resonanceGround state

摘要: Two new azido-bridged polyoxometalate compounds were synthesized in acetonitrile/methanol media and their molecular structures have been determined by X-ray crystallography. The [[(gamma-SiW10O36)Mn2(OH)2(N3)(0.5)(H2O)(0.5)]2(mu-1,3-N3)](10-) (1 a) tetranuclear Mn(III) complex, which an end-to-end N3- ligand acts as a linker between two [(gamma-SiW10O36)Mn2(OH)2]4- units, represents the first manganese-azido polyoxometalate. magnetic properties studied considering spin Hamiltonian H = -J1(S1S2+S1*S2*)-J2(S1S1*), showing that antiferromagnetic interactions paramagnetic centers (g 1.98) occur both through di-(mu-OH) bridge (J1 -25.5 cm(-1)) mu-1,3-azido (J2 -19.6 cm(-1)). [(gamma-SiW10O36)2Cu4(mu-1,1,1-N3)2(mu-1,1-N3)2]12- (2 Cu(II) complex consists of [gamma-SiW10O36Cu2(N3)2]6- subunits connected mu-1,1,1-azido ligands, four forming lozenge. susceptibility data fitted. This reveals ferromagnetic centers, leading to S=2 ground state (H -J1(S1S2+S1*S2*)-J2(S2S2*), J1 +294.5 cm(-1), J2 +1.6 g 2.085). coupling each subunit is strongest ever observed either compound or diazido-bridged complex. Considering 2 previously reported basal-basal di-(mu-1,1-N3)-bridged complexes metallic are not other magnetically linear correlation 2639.5-24.95*theta(av) theta(av) bridging angle parameter has proposed. electronic structure also investigated using multifrequency high-field electron resonance (HF-EPR) spectroscopy 95 285 GHz. parameters S (D -0.135(2) E -0.003(2) g(x) 2.290(5), g(y) 2.135(10), g(z) 2.158(5)) well excited 1 -0.960(4) -0.080(5) 2.042(5), 2.335(5), 2.095(5)) determined, since energy gap these states very small (1.6

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