Zheng Sipeng, Reintjens Niels R M, Siegler Maxime A, Roubeau Olivier, Bouwman Elisabeth, Rudavskyi Andrii, Havenith Remco W A, Bonnet Sylvestre
Leiden Institute of Chemistry, Gorlaeus Laboratories, Leiden University, P.O. Box 9502, Leiden, 2300 RA (The Netherlands).
Small Molecule X-ray Facility, Department of Chemistry, Johns Hopkins University, Baltimore, MD 21218 (USA).
Chemistry. 2016 Jan 4;22(1):331-9. doi: 10.1002/chem.201503119. Epub 2015 Nov 18.
The tetrapyridyl ligand bbpya (bbpya=N,N-bis(2,2'-bipyrid-6-yl)amine) and its mononuclear coordination compound [Fe(bbpya)(NCS)2 ] (1) were prepared. According to magnetic susceptibility, differential scanning calorimetry fitted to Sorai's domain model, and powder X-ray diffraction measurements, 1 is low-spin at room temperature, and it exhibits spin crossover (SCO) at an exceptionally high transition temperature of T1/2 =418 K. Although the SCO of compound 1 spans a temperature range of more than 150 K, it is characterized by a wide (21 K) and dissymmetric hysteresis cycle, which suggests cooperativity. The crystal structure of the LS phase of compound 1 shows strong NH⋅⋅⋅S intermolecular H-bonding interactions that explain, at least in part, the cooperative SCO behavior observed for complex 1. DFT and CASPT2 calculations under vacuum demonstrate that the bbpya ligand generates a stronger ligand field around the iron(II) core than its analogue bapbpy (N,N'-di(pyrid-2-yl)-2,2'-bipyridine-6,6'-diamine); this stabilizes the LS state and destabilizes the HS state in 1 compared with [Fe(bapbpy)(NCS)2 ] (2). Periodic DFT calculations suggest that crystal-packing effects are significant for compound 2, in which they destabilize the HS state by about 1500 cm(-1) . The much lower transition temperature found for the SCO of 2 compared to 1 appears to be due to the combined effects of the different ligand field strengths and crystal packing.
制备了四吡啶基配体bbpya(bbpya = N,N-双(2,2'-联吡啶-6-基)胺)及其单核配位化合物[Fe(bbpya)(NCS)₂ ](1)。根据磁化率、拟合索赖畴模型的差示扫描量热法以及粉末X射线衍射测量结果,1在室温下为低自旋态,并且在异常高的转变温度T₁/₂ = 418 K时表现出自旋交叉(SCO)现象。尽管化合物1的SCO跨越超过150 K的温度范围,但其特征是具有宽(21 K)且不对称的滞后循环,这表明存在协同作用。化合物1的低自旋相的晶体结构显示出强烈的NH⋅⋅⋅S分子间氢键相互作用,这至少部分解释了配合物1中观察到的协同SCO行为。真空条件下的密度泛函理论(DFT)和完全活性空间自洽场二阶微扰理论(CASPT2)计算表明,bbpya配体在铁(II)核周围产生的配体场比其类似物bapbpy(N,N'-二(吡啶-2-基)-2,2'-联吡啶-6,6'-二胺)更强;与[Fe(bapbpy)(NCS)₂ ](2)相比,这使1中的低自旋态稳定,高自旋态不稳定。周期性DFT计算表明,晶体堆积效应对于化合物2很重要,在化合物2中,它们使高自旋态不稳定约1500 cm⁻¹ 。与1相比,2的SCO转变温度低得多,这似乎是由于不同配体场强度和晶体堆积的综合影响。