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首页> 外文期刊>Inorganic Chemistry: A Research Journal that Includes Bioinorganic, Catalytic, Organometallic, Solid-State, and Synthetic Chemistry and Reaction Dynamics >Dicopper(II) metallacyclophanes with oligo(p-phenylene-ethynylene) spacers: Experimental foundations and theoretical predictions on potential molecular magnetic wires
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Dicopper(II) metallacyclophanes with oligo(p-phenylene-ethynylene) spacers: Experimental foundations and theoretical predictions on potential molecular magnetic wires

机译:具有低(对-亚苯基-亚乙炔基)间隔基的双铜金属二环烷酮:潜在分子磁线的实验基础和理论预测

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Two novel double-stranded dicopper(II) metallacyclophanes of formula (nBu_4N)_4[Cu_2(dpeba)_2] ·4MeOH·2Et2O (1) and (nBu_4N) 4[Cu_2(tpeba)_2]·12H2O (2) have been prepared by the CuII-mediated self-assembly of the rigid ('rod-like') bridging ligands N,N′-4,4′-diphenylethynebis(oxamate) (dpeba) and N,N′-1,4-di(4-phenylethynyl)phenylenebis(oxamate) (tpeba), respectively. Single crystal X-ray diffraction analysis of 1 confirms the presence of a dicopper(II)tetraaza[3.3]4,4′-diphenylethynophane metallacyclic structure featuring a very long intermetallic distance between the two square planar CuII ions [r = 14.95(1) ?]. The overall parallel-displaced π-stacked conformation of the two nearly planar para substituted diphenylethyne spacers [dihedral angle (ψ) of 7.8(1)] leads to important deviations from the perpendicular orientation of the copper mean basal planes with respect to the facing benzene planes [dihedral angles (π) of 56.4(1) and 58.4(1)]. X-band EPR spectra together with variable-temperature magnetic susceptibility and variable-field magnetization measurements of 1 and 2, both in solution and in the solid state, show the occurrence of a non-negligible, moderate to weak intramolecular antiferromagnetic coupling [-J = 3.9-4.1 (1) and 0.5-0.9 cm~(-1) (2); H = -JS1·S 2 with S_1 = S_2 = S_(Cu) = 1/2]. Density functional calculations on the BS singlet (S = 0) and triplet (S = 1) spin states of the model complexes 1 and 2 with an ideal orthogonal molecular geometry (ψ = 0 and π = 90) support the occurrence of a spin polarization mechanism for the propagation of the exchange interaction between the two unpaired electrons occupying the d_(xy) orbital of each square planar Cu~(II) ion through the predominantly π-type orbital pathway of the double p-diphenylethyne (1) and di(phenylethynyl)phenylene spacers (2). Time-dependent density functional calculations reproduce the observed bathochromic shift of the main intraligand (IL) π-π* transition in the electronic absorption spectra of 1 and 2 [λ_1 = 308 (1) and 316 nm (2)]. In the series of orthogonal model complexes 1-5 with linear oligo(p-phenylene-ethynylene) (OPE) spacers, -C_6H _4(C? - CC_6H_4)_n- (n = 1-5), a linear increase of the IL π-π* transition energy with the reciprocal of the intermetallic distance is theoretically predicted [ν_(max) = 1.99 × 10~4 + 2.15 × 10~5 (1/r) (S = 0) or ν = 2.01 × 10~4 + 2.18 × 10~5 (1/r) (S = 1)], which clearly indicates that the effective π-conjugation length increases with the number of phenylethyne repeating units. This is accompanied by an exponential decay of the antiferromagnetic coupling with the intermetallic distance [-J = 1.08 × 10~3 exp(-0.31r)], which supports the ability of the extended π-conjugated OPEs to mediate the exchange interaction between the unpaired electrons of the two Cu~(II) centers with intermetallic distances in the range of 1.5-4.3 nm. Further developments may be then envisaged for this new family of oxamato-based dicopper(II) oligo-p-phenylethynophanes on the basis of the unique ligand capacity to act as a molecular antiferromagnetic wire.
机译:制备了两种新型的式(nBu_4N)_4 [Cu_2(dpeba)_2]·4MeOH·2Et2O(1)和(nBu_4N)4 [Cu_2(tpeba)_2]·12H2O(2)的双链双铜金属盐。通过CuII介导的刚性(“棒状”)桥联配体N,N'-4,4'-二苯基乙炔双(草酸酯)和N,N'-1,4-di(4)的自组装-苯基乙炔基)亚苯基双(草酸酯)(tpeba)。 X的单晶X射线衍射分析证实存在dicopper(II)tetraaza [3.3] 4,4'-diphenylethynophane金属环结构,其特征在于两个方形平面CuII离子之间的金属间距离非常长[r = 14.95(1) ?]。两个几乎为平面的对位取代的二苯基乙炔间隔基的整体平行位移π堆叠构型[7.8(1)的二面角(ψ)]导致铜平均基面相对于相对的苯的垂直取向发生重大偏离平面[56.4(1)和58.4(1)的二面角(π)]。 X波段EPR光谱以及在溶液和固态下的可变温度磁化率和1和2的可变场磁化强度测量结果表明,发生了不可忽略的,中等至弱的分子内反铁磁耦合[-J = 3.9-4.1(1)和0.5-0.9 cm〜(-1)(2); H = -JS1·S 2,其中S_1 = S_2 = S_(Cu)= 1/2]。具有理想正交分子几何形状(ψ= 0和π= 90)的模型配合物1和2的BS单重态(S = 0)和三重态(S = 1)自旋态的密度泛函计算支持自旋极化的发生占据每个方形平面Cu〜(II)离子的d_(xy)轨道的两个未配对电子之间的交换相互作用的传播机理,主要通过双对二苯乙炔(1)和di(苯基乙炔基)亚苯基间隔基(2)。随时间变化的密度泛函计算在1和2 [λ_1= 308(1)和316 nm(2)]的电子吸收光谱中再现了观察到的主要配体(IL)π-π*跃迁的红移。在带有线性低聚(对亚苯基亚乙炔基)(OPE)间隔基的正交模型复合物1-5的系列中,-C_6H _4(C2-CC_6H_4)_n-(n = 1-5),IL的线性增加理论上预测了π-π*跃迁能与金属间距离的倒数[ν_(max)= 1.99×10〜4 + 2.15×10〜5(1 / r)(S = 0)或ν= 2.01×10〜 4 + 2.18×10〜5(1 / r)(S = 1)],这清楚地表明有效的π共轭长度随苯乙炔重复单元数的增加而增加。这伴随着反铁磁耦合的指数衰减与金属间距离[-J = 1.08×10〜3 exp(-0.31r)],这支持扩展的π共轭OPE介导了金属之间的交换相互作用。两个Cu〜(II)中心的不成对电子,金属间距离为1.5-4.3 nm。然后,基于独特的配体充当分子反铁磁线的能力,可以为基于恶唑的新家族的双铜(II)低聚对苯基乙炔基苯酚进行进一步的开发。

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