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首页> 外文期刊>CrystEngComm >Synthesis, structure, thermal, magnetic properties and quantum mechanical calculations of bridged [bis(di(2-methylpyridyl)amine)-(μ2-1,2-bis(4-pyridyl)ethane)-tetraperchlorato-dicopper(II)] dihydrate complex
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Synthesis, structure, thermal, magnetic properties and quantum mechanical calculations of bridged [bis(di(2-methylpyridyl)amine)-(μ2-1,2-bis(4-pyridyl)ethane)-tetraperchlorato-dicopper(II)] dihydrate complex

机译:桥联二水合双[二(二(2-甲基吡啶基)胺)-(μ2-1,2-双(4-吡啶基)乙烷)-四氯合-双铜(II)]的合成,结构,热,磁性和量子力学计算复杂

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摘要

The title compound [Cu2(DPA)2(μ-bpe)(ClO4)4]·2H2O, I where DPA = di(2-methylpyridyl)amine and bpe = 1,2-bis(4-pyridyl)ethane was studied by single crystal X-ray crystallography at different temperatures, spectroscopic methods, differential scanning calorimetry (DSC) and by magnetic susceptibility methods. DSC studies were recorded between 125 K and 647 K and magnetic studies between 2 K and 300 K. The X-ray diffraction studies were carried out at 293, 200, 150 and 100 K. Cooling the crystal from 293 K to 100 K produces a significant change in cell constants but no change in space group. X-ray and DSC studies revealed that significant phase transitions occur at temperatures between 200 K and 100 K that are described herein. The X-ray studies revealed a thermally-induced case of polymorphism whereby the cell volume triples on going from 293 to 100 K. This transition was reversible even though there is a marked hysteresis in the process. The major structural change between 200 K and 100 K is due to the displacement of the central bpe pyridyl rings relative to the plane defining CuN1N2N3 and the bending angle Cu-N1-C3. This transitional phase change was indirectly supported by quantum mechanical calculations which indicated the absence of significant π-π stacking interaction between the central bpe pyridyl rings forming the two parallel dinuclear species. This was attributed to the long 8.28 A distances between the two indicated moieties. Lack of energetic and spatial constraints justified the pyridyl ring displacement along the N-C3 axis. The temperature dependence of the magnetic behavior of I was that of a simple paramagnet down to 2 K. The complex revealed a very weak to non-existent magnetic coupling between the Cu(II) centers (J = -0.34 cm~(-1)).
机译:通过以下方法研究了标题化合物[Cu2(DPA)2(μ-bpe)(ClO4)4]·2H2O,其中DPA =二(2-甲基吡啶基)胺和bpe = 1,2-双(4-吡啶基)乙烷在不同温度下的单晶X射线晶体学,光谱方法,差示扫描量热法(DSC)和磁化率方法。 DSC研究记录在125 K和647 K之间,磁研究记录在2 K和300 K之间。X射线衍射研究在293、200、150和100 K下进行。将晶体从293 K冷却到100 K会产生晶体。细胞常数发生显着变化,但空间组没有变化。 X射线和DSC研究表明,本文所述的200 K和100 K之间的温度下会发生明显的相变。 X射线研究揭示了热诱导的多态现象,其中细胞体积从293增加到100 K时增加了三倍。即使此过程中存在明显的滞后现象,这种转变也是可逆的。在200 K和100 K之间的主要结构变化是由于中心bpe吡啶环相对于限定CuN1N2N3的平面和弯曲角度Cu-N1-C3的位移而引起的。量子力学计算间接支持了这种过渡相变,这表明形成两个平行双核物质的中心bpe吡啶基环之间不存在明显的π-π堆积相互作用。这归因于两个所示部分之间的长8.28 A的距离。缺乏能量和空间限制证明了吡啶环沿N-C3轴的位移。 I磁行为的温度依赖性是低至2 K的简单顺磁铁的磁依赖性。该络合物显示Cu(II)中心之间的磁耦合非常弱至不存在(J = -0.34 cm〜(-1) )。

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