新型单体[CoI2(dppfO2)]和聚合链[CoI2(μ-dppfO2)n]的合成、x射线结构、电化学、磁性能及理论研究

T. Avilés, A. Dinis, José Orlando Gonçalves, V. Félix, M. J. Calhorda, Ângela O. Prazeres, M. Drew, H. Alves, R. Henriques, V. Gama, P. Zanello, M. Fontani
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The structural characterisation of compounds 2, 3, and 4 was carried out by single crystal X-ray diffraction studies. The magnetic behaviour of [CoI2(dppfO2)] and [CoI2(μ-dppfO2)]n was studied, and the results are consistent with tetrahedral S \n= 3/2 CoII, possessing a 4A2 ground state, and S \n= 0 FeII. In these compounds, CoII negative zero field splittings were determined from an analysis of the magnetic susceptibility temperature dependence, with D/k \n= \n−13 and −14 K for CoI2(dppfO2) and [CoI2(μ-dppfO2)]n, respectively. DFT calculations were performed in order to understand the electronic structure of [Co(η5-C5H5)(dppf-P,P′)I]I, 1, as well as that of the paramagnetic specie [CoI2(dppfO2)], 4. The [CoI2(μ-dppfO2)]n chain was also analysed and found to behave very similarly to the monomeric iodine derivative 4. The calculations showed the unpaired electrons to be localized on the Co(II) centre in all these species. 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引用次数: 16

摘要

以Co(III)配合物[Co(η - 5- c5h5)(dppf-P,P′)I], 2为原料,与1,1′-二苯基膦二茂铁(dppf)在CH2Cl2中进行化学计量反应,合成了新化合物[Co(η - 5- c5h5)(Co)I2], 2,并用核磁共振谱对其进行了表征。化合物1暴露于四氢呋喃或CH2Cl2溶液的空气中,以一种意想不到的方式,形成一个由桥接1,1 ' -二(氧二苯磷酰)二茂铁(dppfO2)连接四面体Co(II)单元[CoI2(μ-dppfO2)]n, 3组成的聚合链。试图通过dppfO2与CoI2在CH2Cl2中直接反应获得聚合链3,得到单体化合物[CoI2(dppfO2)], 4,其中dppfO2以螯合方式配位。化合物2、3和4的结构表征是通过单晶x射线衍射研究进行的。研究了[CoI2(dppfO2)]和[CoI2(μ-dppfO2)]n的磁性行为,结果与四面体S = 3/2 CoII一致,具有4A2基态,S = 0 FeII。CoI2(dppfO2)和[CoI2(μ-dppfO2)]n的D/k分别为- 13和- 14 k,通过磁化率温度依赖性分析确定了CoII负零场劈裂。为了了解[Co(η5-C5H5)(dppf-P,P′)I]I, 1和顺磁性[CoI2(dppfO2)], 4的电子结构,我们进行了DFT计算。对[CoI2(μ-dppfO2)]n链也进行了分析,发现其行为与单体碘衍生物4非常相似。计算结果表明,未配对电子在所有这些物质中都定位在Co(II)中心。讨论了dppf配合物[CoIII(η - 5- c5h5)(dppf-P,P′)I]和[Co(dppfO2)I2]所表现出的相当复杂的电化学行为。
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Synthesis, X-ray structures, electrochemistry, magnetic properties, and theoretical studies of the novel monomeric [CoI2(dppfO2)] and polymeric chain [CoI2(μ-dppfO2)n]
The new compound [Co(η5-C5H5)(dppf-P,P′)I]I, 1, was synthesised by the stoichiometric reaction of the Co(III) complex [Co(η5-C5H5)(CO)I2], 2, with 1,1′-bis(diphenylphosphino)ferrocene (dppf) in CH2Cl2, and was characterised by multinuclear NMR spectroscopy. Exposure to air of THF or CH2Cl2 solutions of compound 1 gave, in an unexpected way, a polymeric chain comprising bridging 1,1′-bis(oxodiphenylphosphoranyl)ferrocene (dppfO2) joining tetrahedral Co(II) units [CoI2(μ-dppfO2)]n, 3. Attempts to obtain the polymeric chain 3 by the direct reaction of dppfO2 with CoI2, in CH2Cl2, gave instead the monomeric compound [CoI2(dppfO2)], 4, in which dppfO2 is coordinated in a chelating mode. The structural characterisation of compounds 2, 3, and 4 was carried out by single crystal X-ray diffraction studies. The magnetic behaviour of [CoI2(dppfO2)] and [CoI2(μ-dppfO2)]n was studied, and the results are consistent with tetrahedral S = 3/2 CoII, possessing a 4A2 ground state, and S = 0 FeII. In these compounds, CoII negative zero field splittings were determined from an analysis of the magnetic susceptibility temperature dependence, with D/k = −13 and −14 K for CoI2(dppfO2) and [CoI2(μ-dppfO2)]n, respectively. DFT calculations were performed in order to understand the electronic structure of [Co(η5-C5H5)(dppf-P,P′)I]I, 1, as well as that of the paramagnetic specie [CoI2(dppfO2)], 4. The [CoI2(μ-dppfO2)]n chain was also analysed and found to behave very similarly to the monomeric iodine derivative 4. The calculations showed the unpaired electrons to be localized on the Co(II) centre in all these species. The rather complicated electrochemical behaviour exhibited by the dppf complex [CoIII(η5-C5H5)(dppf-P,P′)I]I and by [Co(dppfO2)I2] is discussed.
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