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Slow Magnetic Relaxation in a Family of Trigonal Pyramidal Iron(II) Pyrrolide Complexes

机译:三角金字塔形铁(II)吡咯化物络合物家族中的慢磁弛豫。

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We present a family of trigonal pyramidal iron(II) complexes supported by tris(pyrrolyl-α-methyl)amine ligands of the general formula [M(solv)n][(tpaR)Fe] (M = Na, R = tert-butyl (1), phenyl (4); M = K, R = mesityl (2), 2,4,6-triisopropylphenyl (3), 2,6-difluorophenyl (5)) and their characterization by X-ray crystallography, Mössbauer spectroscopy, and high-field EPR spectroscopy. Expanding on the discovery of slow magnetic relaxation in the recently reported mesityl derivative 2, this homologous series of high-spin iron(II) complexes enables an initial probe of how the ligand field influences the static and dynamic magnetic behavior. Magnetization experiments reveal large, uniaxial zero-field splitting parameters of D = −48, −44, −30, −26, and −6.2 cm−1 for 1−5, respectively, demonstrating that the strength of axial magnetic anisotropy scales with increasing ligand field strength at the iron(II) center. In the case of 2,6-difluorophenyl substituted 5, high-field EPR experiments provide an independent determination of the zero-field splitting parameter (D = −4.397(9) cm−1) that is in reasonable agreement with that obtained from fits to magnetization data. Ac magnetic susceptibility measurements indicate field-dependent, thermally activated spin reversal barriers in complexes 1, 2, and 4 of Ueff = 65, 42, and 25 cm−1, respectively, with the barrier of 1 constituting the highest relaxation barrier yet observed for a mononuclear transition metal complex. In addition, in the case of 1, the large range of temperatures in which slow relaxation is observed has enabled us to fit the entire Arrhenius curve simultaneously to three distinct relaxation processes. Finally, zero-field Mössbauer spectra collected for 1 and 4 also reveal the presence of slow magnetic relaxation, with two independent relaxation barriers in 4 corresponding to the barrier obtained from ac susceptibility data and to the 3D energy gap between the MS = ±2 and ±1 levels, respectively.
机译:我们提出了由通式[M(solv) n ] [(tpa R <的三(吡咯基-α-甲基)胺)配体支撑的一族三角锥铁(II)配合物/ sup>)Fe](M = Na,R =叔丁基(1),苯基(4); M = K,R =甲苯基(2),2,4,6-三异丙基苯基(3),2,6 -二氟苯基(5))及其通过X射线晶体学,穆斯堡尔光谱和高场EPR光谱进行表征。扩展了最近报道的异氰酸酯衍生物2中慢磁弛豫的发现范围,该同源系列的高自旋铁(II)配合物使人们能够初步探究配体场如何影响静态和动态磁行为。磁化实验表明,大的单轴零场分裂参数D = −48,−44,−30,−26和−6.2 cm -1 分别为1–5,表明强度铁(II)中心的轴向磁各向异性尺度随配体场强的增加而增加。在2,6-二氟苯基取代5的情况下,高场EPR实验可独立确定零场分裂参数(D = -4.397(9)cm -1 )与从磁化数据拟合中获得的结果有合理的一致性。交流磁化率测量表明,U eff 的配合物1、2和4 = 65、42和25 cm -1 时,依赖于场的热激活自旋反转势垒,分别以1的势垒构成最高的弛豫势垒,这是单核过渡金属配合物所观察到的。此外,在1的情况下,观察到缓慢弛豫的温度范围很大,这使我们能够同时将整个Arrhenius曲线拟合到三个不同的弛豫过程。最后,针对1和4收集的零场Mösbauer光谱也揭示了慢磁弛豫的存在,其中4个中的两个独立的弛豫势垒对应于从磁化率数据获得的势垒以及Ms之间的3D能隙 =分别为±2和±1。

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