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杂桥联μ-亚硝基-μ(1,1)-叠氮双核镍(II)化合物中的磁交换相互作用和磁结构相关性:实验与理论的综合研究。

Magnetic exchange interactions and magneto-structural correlations in heterobridged μ-phenoxo-μ(1,1)-azide dinickel(II) compounds: a combined experimental and theoretical exploration.

机构信息

Department of Chemistry, University of Calcutta, 92 A. P. C. Road, Kolkata 700 009, India.

出版信息

Inorg Chem. 2011 Aug 1;50(15):7257-67. doi: 10.1021/ic200833y. Epub 2011 Jun 23.

Abstract

This investigation presents the syntheses, crystal structures, magnetic properties, and density functional theoretical modeling of magnetic behavior of two heterobridged μ-phenoxo-μ(1,1)-azido dinickel(II) compounds [Ni(II)(2)(L(1))(2)(μ(1,1)-N(3))(N(3))(H(2)O)]·CH(3)CH(2)OH (1) and Ni(II)(2)(L(2))(2)(μ(1,1)-N(3))(CH(3)CN)(H(2)O)·H(2)O·CH(3)CN (2), where HL(1) and HL(2) are the [1+1] condensation products of 3-methoxysalicylaldehyde and 1-(2-aminoethyl)-piperidine (for HL(1))/4-(2-aminoethyl)-morpholine (for HL(2)), along with density functional theoretical magneto-structural correlations of μ-phenoxo-μ(1,1)-azido dinickel(II) systems. Compounds 1 and 2 crystallize in orthorhombic (space group Pbca) and monoclinic (space group P2(1)/c) systems, respectively. The coordination environments of both metal centers are distorted octahedral. The variable-temperature (2-300 K) magnetic susceptibilities at 0.7 T of both compounds have been measured. The interaction between the metal centers is moderately ferromagnetic; J = 16.6 cm(-1), g = 2.2, and D = -7.3 cm(-1) for 1 and J = 16.92 cm(-1), g = 2.2, and D(Ni1) = D(Ni2) = -6.41 cm(-1) for 2. Broken symmetry density functional calculations of exchange interaction have been performed on complexes 1 and 2 and provide a good numerical estimate of J values (15.8 cm(-1) for 1 and 15.35 cm(-1) for 2) compared to experiments. The role of Ni-N bond length asymmetry on the magnetic coupling has been noted by comparing the structures and J values of complexes 1 and 2 together with previously published dimers 3 (Eur. J. Inorg. Chem. 2009, 4982), 4 (Inorg. Chem. 2004, 43, 2427), and 5 (Dalton Trans. 2008, 6539). Our extensive DFT calculations reveal an important clue to the mechanism of coupling where the orientation of the magnetic orbitals seems to differ with asymmetry in the Ni-N bond lengths. This difference in orientation leads to a large change in the overlap integral between the magnetic orbitals and thus the magnetic coupling. DFT calculations have also been extended to develop several magneto-structural correlations in this type of complexes and the correlation aim to focus on the asymmetry of the Ni-N bond lengths reveal that the asymmetry plays a proactive role in governing the magnitude of the coupling. From a completely symmetric Ni-N bond length, two behaviors have been noted: with a decrease in bond length there is an increase in the ferromagnetic coupling, while an increase in the bond lengths leads to a decrease in ferromagnetic interaction. The later correlation is supported by experiments. The magnetic properties of 1, 2, and three previously reported related compounds have been discussed in light of the structural parameters and also in light of the theoretical correlations determined here.

摘要

本研究介绍了两个异桥联的 μ- 酚氧基-μ(1,1)- 叠氮二镍(II)化合物[Ni(II)(2)(L(1))(2)(μ(1,1)-N(3))(N(3))(H(2)O)]·CH(3)CH(2)OH(1)和Ni(II)(2)(L(2))(2)(μ(1,1)-N(3))(CH(3)CN)(H(2)O)·H(2)O·CH(3)CN(2)的合成、晶体结构、磁性能以及基于密度泛函理论的磁行为建模,其中 HL(1)和 HL(2)是 3-甲氧基水杨醛和 1-(2-氨基乙基)哌啶(用于 HL(1))/4-(2-氨基乙基)吗啉(用于 HL(2))的[1+1]缩合产物。此外,还对 μ- 酚氧基-μ(1,1)- 叠氮二镍(II)体系进行了密度泛函理论磁结构关联。化合物 1 和 2 分别结晶在正交(空间群 Pbca)和单斜(空间群 P2(1)/c)系统中。两个金属中心的配位环境都是变形八面体。在 0.7 T 下测量了两个化合物的变温(2-300 K)磁导率。两个金属中心之间的相互作用是中等程度的铁磁性;J = 16.6 cm(-1),g = 2.2,D = -7.3 cm(-1),对于 1,J = 16.92 cm(-1),g = 2.2,D(Ni1) = D(Ni2) = -6.41 cm(-1),对于 2。对配合物 1 和 2 进行了交换相互作用的非对称密度泛函计算,并与实验结果进行了比较,提供了对 J 值的良好数值估计(J = 15.8 cm(-1),对于 1;J = 15.35 cm(-1),对于 2)。通过比较配合物 1 和 2 的结构和 J 值,并结合以前发表的二聚体 3(Eur. J. Inorg. Chem. 2009, 4982)、4(Inorg. Chem. 2004, 43, 2427)和 5(Dalton Trans. 2008, 6539),注意到 Ni-N 键长不对称性对磁耦合的影响。我们广泛的密度泛函计算为耦合机制提供了一个重要线索,其中磁轨道的取向似乎随 Ni-N 键长的不对称性而不同。这种取向的差异导致磁轨道之间的重叠积分发生很大变化,从而导致磁耦合。密度泛函计算还扩展到这种类型的配合物中建立了几个磁结构关联,关联旨在关注 Ni-N 键长的不对称性,表明不对称性在控制耦合强度方面起着积极的作用。从完全对称的 Ni-N 键长开始,注意到两种行为:随着键长的减小,铁磁耦合增加,而随着键长的增加,铁磁相互作用减小。后者的相关性得到了实验的支持。根据结构参数以及这里确定的理论相关性,讨论了 1、2 和三个以前报道的相关化合物的磁性质。

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