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首页> 外文期刊>Chemistry: A European journal >Constructing single-chain magnets by supramolecular π-π stacking and spin canting: A case study on manganese(III) corroles
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Constructing single-chain magnets by supramolecular π-π stacking and spin canting: A case study on manganese(III) corroles

机译:通过超分子π-π堆叠和自旋倾斜构造单链磁体:以锰(III)腐蚀为例

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摘要

A single-chain magnet (SCM) was constructed from manganese(III) 5,10,15-tris(pentafluorophenyl)corrole complex [Mn ~(III)(tpfc)] through supramolecular π-π stacking without bridging ligands. In the crystal structures, [Mn(tpfc)] molecules crystallized from different solvents, such as methanol, ethyl acetate, and ethanol, exhibit different molecular orientations and intermolecular π-π interaction or weak Mn...O interaction to form a supramolecular one-dimensional motif or dimer. These three complexes show very different magnetic behaviors at low temperature. Methanol solvate 1 shows obvious frequency dependence of out-of-phase alternating-current magnetic susceptibility below 2 K and a magnetization hysteresis loop with a coercive field of 400 Oe at 0.5 K. It is the first example of spin-canted supramolecular single-chain magnet due to weak π-π stacking interaction. By fitting the susceptibility data χ MT (20-300 K) of 1 with the spin Hamiltonian expression H→=-2J∑ ~(n-1) i=1S→ _(Ai)S→ _(Ai+1)+D∑S→ _(iZ) ~2, the intrachain magnetic coupling parameter transmitted by π-π interaction of -0.31 cm -1 and zero field splitting parameter D of -2.59 cm ~(-1) are obtained. Ethyl acetate solvate 2 behaves as an antiferromagnetic chain without ordering or slow magnetic relaxation down to 0.5 K. The magnetic susceptibility data χ _MT (20-300 K) of 2 was fitted by assuming the spin Hamiltonian H→=-2J∑ ~(n-1) _(i=1)S→ _(Ai)S→ _(Ai+1), and the intrachain antiferromagnetic coupling constant of -0.07 cm ~(-1) is much weaker than that of 1. Ethanol solvate 3 with a dimer motif shows field-induced single-molecule magnet like behavior below 2.5 K. The exchange coupling constant J within the dimer propagated by π-π interaction is -0.14 cm -1 by fitting the susceptibility data χ _MT (20-300 K) with the spin Hamiltonian H→=- 2JS→ _AS→ _B+β(S→ _Ag _A+S→ _Bg _B)H. The present studies open a new way to construct SCMs from anisotropic magnetic single-ion units through weak intermolecular interactions in the absence of bridging ligands. Supramolecular magnets: Manganese(III) 5,10,15-tris(pentafluorophenyl)corrole [Mn ~(III)(tpfc)] forms chains or dimers depending on whether it was crystallized from methanol, ethyl acetate, or ethanol. Due to intermolecular π-π interactions, the depicted methanol solvate [Mn(tpfc)(MeOH)] ·H _2O forms a new type of supramolecular spin-canted single-chain magnet without any bridging ligands.
机译:由锰(III)5,10,15-三(五氟苯基)甲氧基络合物[Mn〜(III)(tpfc)]通过超分子π-π堆积而无需连接配体构成。在晶体结构中,从不同溶剂(例如甲醇,乙酸乙酯和乙醇)中结晶的[Mn(tpfc)]分子表现出不同的分子取向和分子间π-π相互作用或弱Mn ... O相互作用,形成超分子分子维主题或二聚体。这三种络合物在低温下显示出非常不同的磁行为。甲醇溶剂化物1在2 K以下具有明显的频率异相交流磁化率依赖性,在0.5 K时具有400 Oe的矫顽场的磁化磁滞回线。这是自旋倾斜超分子单链的第一个例子由于弱的π-π堆叠相互作用而产生的磁铁。通过用自旋哈密顿表达式H→= -2J∑〜(n-1)i = 1S→_(Ai)S→_(Ai + 1)+ D拟合1的敏感性数据χMT(20-300 K)求得∑S→_(iZ)〜2,通过-0.31cm -1的π-π相互作用传递的链内磁耦合参数和-2.59cm〜(-1)的零场分裂参数D。乙酸乙酯溶剂化物2表现为反铁磁链,无序或缓慢至低至0.5 K的磁弛豫。2的磁化率数据χ_MT(20-300 K)通过假设自旋哈密顿量H→= -2J∑〜(n -1)_(i = 1)S→_(Ai)S→_(Ai + 1),-0.07 cm〜(-1)的链内反铁磁耦合常数比1弱得多。乙醇溶剂化物3具有二聚体基序的分子在2.5 K以下显示出场诱导的单分子磁体样行为。通过拟合磁化率数据χ_MT(20-300 K,通过π-π相互作用传播的二聚体中的交换耦合常数J为-0.14 cm -1 )自旋哈密顿量H→=-2JS→_AS→_B +β(S→_Ag _A + S + _Bg _B)H。本研究开辟了一种新方法,可以在没有桥联配体的情况下通过弱分子间相互作用从各向异性磁性单离子单元构建SCM。超分子磁体:锰(III)5,10,15-三(五氟苯基)甲氧基[Mn〜(III)(tpfc)]取决于其是从甲醇,乙酸乙酯还是乙醇中结晶而形成链或二聚体。由于分子间的π-π相互作用,所描绘的甲醇溶剂化物[Mn(tpfc)(MeOH)]·H _2O形成了一种新型的超分子自旋倾斜单链磁体,没有任何桥联配体。

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