基于丙酮酸硫代氨基甲酸配体的中性铁(III)复合物水合物,具有 T1/2=340 K 的突然自旋交叉和 45 K 的宽滞后环

IF 4.3 3区 材料科学 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC ACS Applied Electronic Materials Pub Date : 2024-11-08 DOI:10.1039/d4dt02901a
Maxim Andreevich Blagov, Alexander V. Akimov, Anatoly S Lobach, Leokadiya Zorina, Sergey Simonov, Konstantin Zakharov, Alexander Vasiliev, Natalia Spitsyna
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引用次数: 0

摘要

利用傅立叶变换红外光谱、粉末和单晶 X 射线衍射、直流电磁测量、EPR 和 57Fe Mössbauer 光谱,合成并表征了基于丙酮酸硫代氨基甲酸配体 [FeIII(Hthpy)(thpy)]-H2O (1)的中性铁(III)配合物水合物。首次确定了 1 的晶体结构。两种不同的螯合配体 Hthpyˉ 和 thpy2ˉ 与铁(III)离子配位,形成 FeN2O2S2 八面体,在 150-350 K 时呈现低自旋几何形状。沿着链,铁络合物的 π-π 相互作用对通过 H 键连接在一起。根据直流磁性测量结果,在 300-363 K 的温度范围内,会出现半转变温度 T1/2=340 K 的完全突然自旋交叉和 45 K 的滞后环。根据 1 的 X 射线结构,孤立二聚体模型的 Bleaney-Bowers 方程被用来近似计算磁感应强度在 2-50 K 范围内的温度依赖性。定义的二聚体内交换常数 Jexp= -0.498(1) K 相当于铁(III)磁中心之间的弱反铁磁交换。对 1 晶体结构中 HS 和 LS 状态下的 H- 和 π-π 键片段进行了 DFT 计算。此外,BS-DFT 计算证实了铁络合物的 π-π 键对中存在反铁磁交换 Jcalc = - 0.92 K,并通过计算的自旋密度分布显示了铁(III)离子之间的交换途径。
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Hydrate of neutral iron(III) complex based on pyruvic acid thiosemicarbazone ligand with abrupt spin-crossover with T1/2=340 K and wide hysteresis loop of 45 K
The hydrate of neutral iron(III) complex based on pyruvic acid thiosemicarbazone ligand [FeIII(Hthpy)(thpy)]·H2O (1) was synthesized and characterized using FT-IR spectroscopy, powder and single-crystal X-ray diffraction, dc magnetic measurements, EPR and 57Fe Mössbauer spectroscopy. The crystal structure of 1 was determined for the first time. Two distinct chelating ligands Hthpyˉ and thpycoordinate the Fe(III) ion to form the FeN2O2S2 octahedron which shows a low spin geometry at 150-350 K. The crystal packing contains infinite chains of the Fe(III) complexes as well as water molecules located in cavities. Along the chain, π-π interacting pairs of the Fe complexes are linked by H-bonding. According to the dc magnetic measurements, the complete abrupt spin-crossover with half-transition temperature T1/2=340 K and a hysteresis loop of 45 K occurs in the temperature range of 300‒363 K. Based on the X-ray structure of 1, the Bleaney–Bowers equation for the isolated dimer model was used to approximate the temperature dependence of the magnetic susceptibility in the range of 2–50 K. The defined intradimer exchange constant Jexp= −0.498(1) K corresponds to a weak antiferromagnetic exchange between the iron(III) magnetic centers. DFT calculations of H- and π-π bonded fragments of the crystal structure of 1 in the HS and LS states were carried out. Moreover, BS-DFT calculations confirm the presence of antiferromagnetic exchange Jcalc = – 0.92 K in the π-π bonded pairs of the ferric complexes, and show the exchange pathway between Fe(III) ions by the calculated spin density distribution.
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