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Synthesis, Structure, Luminescent, and Magnetic Properties of Carbonato-Bridged ZnII2LnIII2 Complexes [(渭4-CO3)2{ZnII<
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Carbonato-bridged ZnII2LnIII2 complexes [(渭4-CO3)2{ZnIILnLnIII(NO3)}2]路solvent were synthesized through atmospheric CO2 fixation reaction of [ZnIILn(H2O)2]路xH2O, LnIII(NO3)3路6H2O, and triethylamine, where LnIII = GdIII, TbIII, DyIII; L1 = N,N鈥?bis(3-methoxy-2-oxybenzylidene)-1,3-propanediaminato, L2 = N,N鈥?bis(3-ethoxy-2-oxybenzylidene)-1,3-propanediaminato. Each ZnII2LnIII2 structure possessing an inversion center can be described as two di-渭-phenoxo-bridged {ZnIILnLnIII(NO3)} binuclear units bridged by two carbonato CO32鈥?/sup> ions. The ZnII ion has square pyramidal coordination geometry with N2O2 donor atoms of Ln and one oxygen atom of a bridging carbonato ion at the axial site. LnIII ion is coordinated by nine oxygen atoms consisting of four from the deprotonated Schiff-base Ln, two from a chelating nitrate, and three from two carbonate groups. The temperature-dependent magnetic susceptibilities in the range 1.9鈥?00 K, field-dependent magnetization from 0 to 5 T at 1.9 K, and alternating current magnetic susceptibilities under the direct current bias fields of 0 and 1000 Oe were measured. The magnetic properties of the ZnII2LnIII2 complexes are analyzed on the basis of the dicarbonato-bridged binuclear LnIII鈥揕nIII structure, as the ZnII ion with d10 electronic configuration is diamagnetic. ZnGd1 (L1) and ZnGd2 (L2) show a ferromagnetic GdIII鈥揋dIII interaction with J(Gd鈥揋d) = +0.042 and +0.028 cm鈥?, respectively, on the basis of the Hamiltonian H = 鈭?J(Gd鈥揋d)Gd1Gd2. The magnetic data of the ZnII2LnIII2 complexes (LnIII = TbIII, DyIII) were analyzed by a spin Hamiltonian including the crystal field effect on the LnIII ions and the LnIII鈥揕nIII magnetic interaction. The Stark splitting of the ground state was so evaluated, and the energy pattern indicates a strong easy axis (Ising type) anisotropy. Luminescence spectra of ZnII2TbIII2 complexes were observed, while those of ZnII2DyIII2 were not detected. The fine structure assignable to the 5D4 鈫?7F6 transition of ZnTb1 and ZnTb2 is in good accord with the energy pattern from the magnetic analysis. The ZnII2LnIII2 complexes (LnIII = TbIII, DyIII) showed an out-of-phase signal with frequency-dependence in alternating current susceptibility, indicative of single molecule magnet. Under a dc bias field of 1000 Oe, the signals become significantly more intense and the energy barrier, 螖/kB, for the magnetic relaxation was estimated from the Arrhenius plot to be 39(1) and 42(8) K for ZnTb1 and ZnTb2, and 52(2) and 67(2) K for ZnDy1 and ZnDy2, respectively.

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