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Metallic coordination selectivity effect in the trinuclear M3(RCOO)6 secondary building units of three layer metal–carboxylate frameworks

机译:三层金属 - 羧酸骨框架三层M3(RCOO)6二级建筑单元中的金属配位选择性效果

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Three two-dimensional metal–carboxylate frameworks (MCFs), namely Zn _(3) (BDC) _(3) (py) _(2) ·2DMF ( 1 ), Mn _(3) (BDC) _(3) (DMF) _(4) ( 2 ) and Co _(3) (BDC) _(3) (DMF) _(2) (py) _(2) ( 3 ) [H _(2) BDC = 1,4-benzene dicarboxylic acid, py = pyridine, DMF = N , N ′-dimethylformamide], have been synthesized by reaction of the M(NO _(3) ) _(2) and H _(2) BDC with py as base and DMF as solvent, under the microwave-assisted solvo-thermal conditions. Three MCFs were characterized by single crystal X-ray diffraction and mensurated its fluorescent or magnetic behaviors. The structural analyses reveal that 1–3 are constructed of the slightly dissimilar carboxylate bridged linear M _(3) (RCOO) _(6) (L _(T) ) _(2/4) clusters where the coordination terminal ligand (L _(T) ) are py in 1 , DMF in 2 and py/DMF in 3 , respectively. The results demonstrated the different metal ions in two side of every SBU inclined to coordinate their respectively selected L _(T) . The time-dependent density functional theory (TDDFT) calculations of 1 show that the emission peak of 423–428 nm (the experimental value is 425 nm) might be derived from the energy transition on the ligand-to-ligand charge transfer (LLCT) where electron densities residing on the π-bonding orbital of BDC ~(2?) are transferred to the π*-anti-bonding orbital of pyridine. Variable-temperature magnetic susceptibility studies indicate the presence of antiferromagnetic exchange coupling within the M _(3) -units of 2 and 3 .
机译:三维二维金属 - 羧酸框架(MCF),即Zn _(3)(BDC)_(3)(PY)_(PY)_(2)·2DMF(1),Mn _(3)(BDC)_(3) (DMF)_(4)(2)和CO _(3)(BDC)_(3)(DMF)_(2)(PY)_(PY)_(PY)_(PY)_(2)(3)[H _(2)BDC = 1, 4-苯二羧酸,Py =吡啶,DMF = N,N'-二甲基甲酰胺]通过M(NO _(3))和H _(2)BDC作为基础的反应合成和DMF作为溶剂,在微波辅助溶剂 - 热条件下。通过单晶X射线衍射特征三个MCF并将其荧光或磁性行为呈现。结构分析揭示了1-3由略微不同的羧酸桥桥接线性M _(3)(RCOO)_(6)(L _(T))_(2/4)簇构成,其中配位终端配体(L _(t))分别为1,dmf中的2和py / dmf,分别为3。结果表明,每个SBU的两侧的不同金属离子倾向于坐标分别选择的L _(t)。依赖于时间的密度函数理论(TDDFT)计算的1显示,423-428nm的发射峰(实验值为425nm)可能来自配体与配体电荷转移(L1ct)上的能量转变其中驻留在BDC〜(2?)的π键合轨道上的电子密度转移到吡啶的π* - anti键合轨道上。可变温度磁性敏感性研究表明,在M _(3) - 单和3的M _(3)中存在反铁磁体交换偶联。

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