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Spin States of Homochiral and Heterochiral Isomers of Fe(PyBox)2 2+ Derivatives

机译:Fe(Pybox)2 2+衍生物的旋转状态和Fe(pybox)2 2+衍生物的旋转状态

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摘要

The following iron(II) complexes of 2,6-bis(oxazolinyl)pyridine (PyBox; LH) derivatives are reported: [Fe(LH)2][ClO4]2 (1); [Fe((R)-LMe)2][ClO4]2 ((R)-2; LMe=2,6-bis{4-methyloxazolinyl}pyridine); [Fe((R)-LPh)2][ClO4]2 ((R)-3) and [Fe((R)-LPh)((S)-LPh)][ClO4]2 ((RS)-3; LPh=2,6-bis{4-phenyloxazolinyl}pyridine); and [Fe((R)-LiPr)2][ClO4]2 ((R)-4) and [Fe((R)-LiPr)((S)-LiPr)][ClO4]2 ((RS)-4; LiPr=2,6-bis{4-isopropyloxazolinyl}pyridine). Solid (R)-3⋅MeNO2 exhibits an unusual very gradual, but discontinuous thermal spin-crossover with an approximate Tmath formula of 350 K. The discontinuity around 240 K lies well below Tmath formula , and is unconnected to a crystallographic phase change occurring at 170 K. Rather, it can be correlated with a gradual ordering of the ligand conformation as the temperature is raised. The other solid compounds either exhibit spin-crossover above room temperature (1 and (RS)-3), or remain high-spin between 5–300 K [(R)-2, (R)-4 and (RS)-4]. Homochiral (R)-3 and (R)-4 exhibit more twisted ligand conformations and coordination geometries than their heterochiral isomers, which can be attributed to steric clashes between ligand substituents [(R)-3]; or, between the isopropyl substituents of one ligand and the backbone of the other ((R)-4). In solution, (RS)-3 retains its structural integrity but (RS)-4 undergoes significant racemization through ligand redistribution by 1H NMR. (R)-4 and (RS)-4 remain high-spin in solution, whereas the other compounds all undergo spin-crossover equilibria. Importantly, Tmath formula for (R)-3 (244 K) is 34 K lower than for (RS)-3 (278 K) in CD3CN, which is the first demonstration of chiral discrimination between metal ion spin states in a molecular complex.
机译:报道了以下2,6-双(恶唑啉基)吡啶(PyBox; LH)衍生物的铁(II)配合物:[Fe(LH)2] [ClO 4] 2(1); [Fe(LH)2] [ClO 4] 2(1)。 [Fe((R)-LMe)2] [ClO4] 2((R)-2; LMe = 2,6-双{4-甲基恶唑啉基}吡啶); [Fe((R)-LPh)2] [ClO4] 2((R)-3)和[Fe((R)-LPh)((S)-LPh)] [ClO4] 2((RS)-3 ; LPh = 2,6-双{4-苯基恶唑啉基}吡啶);和[Fe((R)-LiPr)2] [ClO4] 2((R)-4)和[Fe((R)-LiPr)((S)-LiPr)] [ClO4] 2((RS)- 4; LiPr = 2,6-双{4-异丙基恶唑啉基}吡啶)。固体(R)-3⋅MeNO2表现出异常的非常缓慢的但不连续的热自旋交叉,其Tmath公式约为350 K. 240 K左右的不连续性远低于Tmath公式,并且与发生在90℃的晶体相变无关170 K.而是可以将其与温度升高时配体构象的逐渐排序相关联。其他固体化合物在室温以上(1和(RS)-3)表现出自旋交叉,或在5–300 K [[R)-2,(R)-4和(RS)-4之间保持高自旋]。同型(R)-3和(R)-4的杂手性异构体比其杂手性异构体具有更多的扭曲配体构象和配位几何结构,这可归因于配体取代基之间的空间碰撞[[R] -3];或在一个配体的异丙基取代基和另一个配体的主链之间((R)-4)。在溶液中,(RS)-3保持其结构完整性,但(RS)-4通过1H NMR通过配体重新分布而经历显着的消旋作用。 (R)-4和(RS)-4在溶液中保持高自旋,而其他化合物均经历自旋交叉平衡。重要的是,CD3CN中(R)-3(244 K)的Tmath公式比(RS)-3(278 K)的Tmath公式低34 K,这是分子复合物中金属离子自旋态之间手性区分的第一个证明。

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