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首页> 外文期刊>Comptes Rendus Chimie >II 2Fe III 2] 2+ molecular switches: [Fe II(bik) 2(N–) 2] spin-crossover complexes containing [Fe III(Tp)(CN) 3] metalloligands as N-donor]]>
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II 2Fe III 2] 2+ molecular switches: [Fe II(bik) 2(N–) 2] spin-crossover complexes containing [Fe III(Tp)(CN) 3] metalloligands as N-donor]]>

机译:<!“POST”> III 2 ] 2 + 分子交换机:[fe II (bik) 2 (n-)] - metalligands作为n-onor]]>

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摘要

Three novel mixed valence cyanide-bridged {FeIII2FeII2} square complexes were obtained through the self-assembling of [FeIII(Tp)(CN)3]-or [FeIII(Tp*)(CN)3]?cyanido building blocks with thein situformed [FeII(bik)2(S)2] complex (Tp = hydrotris (pyrazol-1-yl)borate, Tp* = hydrotris (3,5-dimethyl-pyrazol-1-yl)borate, bik = bis(1-methylimidazol-2-yl)ketone, S = solvent). The structures of these three complexes (2, 3and4) are reminiscent of that of our previously published square complex {[FeIII(Tp)(CN)3]2[FeII(bik)2]2}·[FeIII(Tp)(CN)3]2·18H2O·4CH3OH (1). They consist of cyanide-bridged square dicationic complexes, ClO4?(2and3) or BF4?(4) counterions and solvate molecules. The FT-IR cyanide stretching vibrations observed at νCN≈ 2145–60?cm?1are typical of {FeIII–CN–FeII} moieties. The investigation of the magnetic properties of2reveals the occurrence of spin-crossover centered atT1/2= 227?K. The χMTvariation,ca. 7?cm3?mol?1?K, reflects the complete spin-state change occurring on both {FeII(bik)(–NC)2} moieties (–NC represents the cyanido building blocks). The Slichter–Drickamer model leads to a weak cooperativity factor, Γ = 1.6?kJ?mol?1(with Γ < 2RT1/2), which reflects the gradual spin-state change. This is in agreement with the molecular structure of2, which does not present significant intermolecular interactions. The calculated enthalpy and entropy variations associated with the spin-state equilibrium are ΔH= 24?kJ?mol?1and ΔS= 105?J?K?1?mol?1. In contrast,3and4show only partial spin-crossover in the accessible temperature range (2–400?K) as theT1/2are shifted toward higher temperatures (ca.T1/2> 400?K). Although no photomagnetic effect is observed for3, compound4shows a moderate increase in the magnetization upon irradiation at low temperature. This phenomenon is ascribed to the light-induced excited spin-state trapping (LIESST) effect. Interestingly, the complex2also shows a remarkable LIESST effect, which is observed with different laser lights covering the visible and near-infrared range. The resulting χMTvalue obtained in the photoinduced state suggests the occurrence of a ferromagnetic interaction inside the {FeIII–CN–FeII} units.
机译:通过[FeIII(TP)(CN)3] --OR [Feiii(TP *)(CN)3]的自组装获得三种新的混合价氰化{FeiII2Feii2}方形复合物[Feii(Bik)2]复合物(TP =水溶式(吡唑-1-基)硼酸硼,TP * =水溶式(3,5-二甲基 - 吡唑-1-基)硼酸硼,BIK = BIS(1-甲基咪唑-2-基)酮,S =溶剂)。这三种复合物(2,3和4)的结构使我们先前公布的方形复合物([FeIII(TP)(CN)3] 2 [FeII(Bik)2] 2}} [Feiii(TP)(CN )3] 2·18H2O·4CH3OH(1)。它们由氰化物桥接正方形络合物,CLO4(2和3)或BF4?(4)抗衡离子和溶剂化物分子组成。在νCN≈1145-60α中观察到的FT-IR氰化物伸展振动?1典型的{feiii-cn-feii}部分。调查磁性的2REVEALS的发生旋转中心att1 / 2 =227Ω·k。 χmtvariation,CA。 7?mol?1?k,反映在{feii(bik)( - nc)2}部分(-nc代表Cyanido构建块)上发生的完全自旋状态变化。 Slichter-Drickamer模型导致弱合作因子,γ= 1.6?KJ?1(具有γ<2RT1 / 2),其反映了逐渐旋转状态的变化。这与2的分子结构一致,其不存在显着的分子间相互作用。与旋转状态平衡相关的计算的焓和熵变化是ΔH=24Ω·kj?mol?1和Δs=105≤j≤k≤1≤mol≤1。相比之下,3AMAW仅在可接近的温度范围内(2-400Ωk)中的部分旋转交叉,如THET1 / 2位于更高的温度(CA.T1 / 2> 400?K)。尽管没有观察到光磁效果3,但在低温下照射时,化合物4显示磁化的中等增加。这种现象归因于光诱导的激发旋转状态捕获(Liesst)效应。有趣的是,复杂的2.Also显示出一种显着的Liesst效果,其用不同的激光灯覆盖可见光和近红外范围。在光导状态下获得的所得χMTValue表明{Feiii-CN-FEII}单元内的铁磁相互作用的发生。

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