Department of Chemistry and The MacDiarmid Institute for Advanced Materials and Nanotechnology, University of Otago, P.O. Box 56, Dunedin 9054, New Zealand.
Inorg Chem. 2011 May 16;50(10):4586-97. doi: 10.1021/ic200308k. Epub 2011 Apr 20.
Seven diiron(II) complexes, Fe(II)(2)(PMAT)(2)(4), varying only in the anion X, have been prepared, where PMAT is 4-amino-3,5-bis{[(2-pyridylmethyl)-amino]methyl}-4H-1,2,4-triazole and X = BF(4)(-) (1), Cl(-) (2), PF(6)(-) (3), SbF(6)(-) (4), CF(3)SO(3)(-) (5), B(PhF)(4)(-) (6), and C(16)H(33)SO(3)(-) (7). Most were isolated as solvates, and the microcrystalline ([3], [4]·2H(2)O, [5]·H(2)O, and [6]·½MeCN) or powder ([2]·4H(2)O, and [7]·2H(2)O) samples obtained were studied by variable-temperature magnetic susceptibility and Mössbauer methods. A structure determination on a crystal of [2]·2MeOH·H(2)O, revealed it to be a [LS-HS] mixed low spin (LS)-high spin (HS) state dinuclear complex at 90 K, but fully high spin, [HS-HS], at 293 K. In contrast, structures of both [5]·¾IPA·H(2)O and [7]·1.6MeOH·0.4H(2)O showed them to be [HS-HS] at 90 K, whereas magnetic and Mössbauer studies on [5]·H(2)O and [7]·2H(2)O revealed a different spin state, [LS-HS], at 90 K, presumably because of the difference in solvation. None of these complexes undergo thermal spin crossover (SCO) to the fully LS form, [LS-LS]. The PF(6)(-) and SbF(6)(-) complexes, 3 and [4]·2H(2)O, appear to be a mixture of [HS-LS] and [HS-HS] at low temperature, and undergo gradual SCO to [HS-HS] on warming. The CF(3)SO(3)(-) complex [5]·H(2)O undergoes gradual, partial SCO from [HS-LS] to a mixture of [HS-LS] and [HS-HS] at T(1/2) ≈ 180 K. The B(PhF)(4)(-) and C(16)H(33)SO(3)(-) complexes, [6]·(1)/(2)MeCN and [7]·2H(2)O, are approximately [LS-HS] at all temperatures, with an onset of gradual SCO with T(1/2) > 300 K.
七种二铁(II)配合物,Fe(II)(2)(PMAT)(2)(4),仅在阴离子 X 上有所不同,已被制备,其中 PMAT 是 4-氨基-3,5-双{[(2-吡啶甲基)-氨基]甲基}-4H-1,2,4-三唑,X 为 BF(4)(-) (1)、Cl(-) (2)、PF(6)(-) (3)、SbF(6)(-) (4)、CF(3)SO(3)(-) (5)、B(PhF)(4)(-) (6)和 C(16)H(33)SO(3)(-) (7)。大多数是作为溶剂化物分离出来的,获得的微晶([3]、[4]·2H(2)O、[5]·H(2)O 和[6]·½MeCN)或粉末([2]·4H(2)O 和[7]·2H(2)O)样品通过变温磁化率和穆斯堡尔方法进行了研究。对[2]·2MeOH·H(2)O 晶体的结构测定表明,在 90 K 时,它是一种[LS-HS]混合低自旋(LS)-高自旋(HS)双核配合物,但在 293 K 时完全是高自旋[HS-HS]。相比之下,[5]·¾IPA·H(2)O 和[7]·1.6MeOH·0.4H(2)O 的结构表明,它们在 90 K 时均为[HS-HS],而对[5]·H(2)O 和[7]·2H(2)O 的磁性和穆斯堡尔研究表明,在 90 K 时,它们具有不同的自旋状态[LS-HS],这可能是由于溶剂化的差异。这些配合物均未发生热自旋交叉(TSC)到完全低自旋[LS-LS]形式。PF(6)(-)和 SbF(6)(-)配合物 3 和[4]·2H(2)O 在低温下似乎是[HS-LS]和[HS-HS]的混合物,并在升温过程中逐渐向[HS-HS]转变。CF(3)SO(3)(-)配合物[5]·H(2)O 逐渐发生部分 TSC,从[HS-LS]到[HS-LS]和[HS-HS]的混合物,在 T(1/2)≈180 K 左右。B(PhF)(4)(-)和 C(16)H(33)SO(3)(-)配合物[6]·(1)/(2)MeCN 和[7]·2H(2)O 在所有温度下均近似为[LS-HS],在 T(1/2)>300 K 时逐渐发生 TSC。