首页> 外文期刊>Inorganica Chimica Acta >Rational design of a new class of heterobimetallic molecule-based magnets: Synthesis, crystal structures, and magnetic properties of oxamato-bridged M-3 ' M-2 (M ' = Li-I and Mn-II; M = Ni-II and Co-II) open-frameworks with a three-dimensional honeycomb architecture
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Rational design of a new class of heterobimetallic molecule-based magnets: Synthesis, crystal structures, and magnetic properties of oxamato-bridged M-3 ' M-2 (M ' = Li-I and Mn-II; M = Ni-II and Co-II) open-frameworks with a three-dimensional honeycomb architecture

机译:新型基于异双金属分子的磁体的合理设计:恶唑桥M-3'M-2(M'= Li-I和Mn-II; M = Ni-II和Co-II)具有三维蜂窝结构的开放式框架

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Two new series of oxamato-bridged heterobimetallic coordination networks of general formula Li-5[Li3M2(mpba)(3)(H2O)(6)] center dot 31H(2)O [M= Ni-II (1a) and Co-II (1b)] and Li-2[Mn3M2(mpba)(3)(H2O)(6)] center dot 22H(2)O [M = Ni-II (2a) and Co-II (2b)] have been prepared from the metal- mediated self-assembly of the hexakis(bidentate), triple-stranded dinickel(I) and dicobalt(II) complexes [M-2(mpba)(3)](8) [mpba = meta-phenylenebis(oxamato)] with either monovalent lithium(I) or divalent manganese(II) ions respectively, in water. X-ray structural analyses of 1a and 1b show an anionic three-dimensional network formed by an infinite parallel array of oxamato-bridged (Li3M2II)-M-I (M = Ni and Co) hexagonal layers, which are interconnected through three m-phenylenediamidate bridges between the M-II ions of opposite propeller chirality (Lambda and Lambda) to give dinuclear metallacrypt and cores of the meso-helicate-type. The intralayer Li-M distance through the oxamate bridge is 5.380(3) (1a) and 5.396(5) (1b) angstrom, while the interlayer M-M distance through the triple m-phenylenediamidate bridge is 6.856(3) (1a) and 6.851(3) (1b) angstrom. Overall, this leads to an open-framework honeycomb structure with large hexagonal pores of ca. 21.8 (1a) and 21.5 angstrom (1b) in diameter which are occupied by linear arrays of water-bridged Li-I countercations. Variable-temperature (2.0-300 K) dc magnetic susceptibility and variable-field (0-5.0 T) magnetization measurements on these two series of compounds reveal a distinct magnetic behavior mainly depending on the diamagnetic or paramagnetic nature of the Li-I and Mn-II ions, respectively. Compounds 1a and 1b behave as rather well-isolated MI2II (M = Ni and Co) dimers with a moderate to weak ferromagnetic coupling(J(Ni-Ni) = + 3.17 cm (1) and J(Co-Co) = + 1.03 cm (1)) between the two M-II ions across the triple m-phenylenediamidate bridge, together with either an appreciable to remarkable local ion axial magnetic anisotropy (D-Ni = -3.35 cm (1)) or spin-orbit coupling (lambda(Co) = - 167.3 cm (1)); the next nearest-neighbor magnetic interactions between the M-II ions through the diamagnetic Li-I ions are negligible. Compounds 2a and 2b behave instead as strongly coupled oxamato-bridged (Mn3M2II)-M-II (M = Ni and Co) ferrimagnetic planes which are weakly interacting through the m-phenylenediamidate bridges, leading thus to a long-range 3D ferromagnetic order at T-C = 6.5 K. In addition, the variable-temperature (2.0-12 K) ac magnetic susceptibility measurements on 2a and 2b show an intriguing frequency-dependent magnetic behavior characteristic of a spin-glass dynamics. This glassy behavior is likely attributed to their amorphous character and/or the moderate to strong magnetic anisotropy of the dinickel(II) and dicobalt(II) precursors.
机译:通式为Li-5 [Li3M2(mpba)(3)(H2O)(6)]中心点31H(2)O [M = Ni-II(1a)和Co- II(1b)]和Li-2 [Mn3M2(mpba)(3)(H2O)(6)]中心点22H(2)O [M = Ni-II(2a)和Co-II(2b)]由六(双齿),三链二镍(I)和二钴(II)配合物[M-2(mpba)(3)](8)的金属介导自组装制备[mpba =间亚苯基(( oxamato)]分别与一价锂(I)或二价锰(II)离子在水中。对1a和1b的X射线结构分析显示了由3个间苯二甲酰胺基桥相互连接的无限长平行的草酰胺桥连的(Li3M2II)-MI(M = Ni和Co)六角形层形成的阴离子三维网络螺旋桨手性相反的M-II离子(Lambda和Lambda)之间形成双核金属隐窝和中螺旋形核。通过草酸酯桥的层内Li-M距离为5.380(3)(1a)和5.396(5)(1b)埃,而通过三联间苯二甲酰胺桥的层间MM距离为6.856(3)(1a)和6.851 (3)(1b)埃。总的来说,这导致了一个开放框架的蜂窝状结构,具有大约六边形的大六边形孔。直径为21.8(1a)和21.5埃(1b),它们被水桥连的Li-I抗衡阳离子的线性阵列占据。对这两个系列化合物的可变温度(2.0-300 K)直流磁化率和可变场(0-5.0 T)磁化强度测量显示出明显的磁行为,这主要取决于Li-I和Mn的反磁或顺磁性质-II离子。化合物1a和1b表现为完全隔离的MI2II(M = Ni和Co)二聚体,具有中等至弱的铁磁耦合(J(Ni-Ni)= + 3.17 cm(1)和J(Co-Co)= + 1.03跨三联间苯二甲酸酯桥的两个M-II离子之间的距离(cm)(1)),或者明显的局部离子轴向磁各向异性(D-Ni = -3.35 cm(1))或自旋轨道耦合( lambda(Co)=-167.3厘米(1));在M-II离子之间通过反磁性Li-I离子之间的下一个最邻近的磁相互作用可以忽略不计。相反,化合物2a和2b表现为强耦合的恶性原子桥接的(Mn3M2II)-M-II(M = Ni和Co)亚铁磁平面,它们通过间苯二甲酰胺桥弱相互作用,从而导致在3D处有长距离3D铁磁有序TC = 6.5K。此外,在2a和2b上的可变温度(2.0-12 K)交流磁化率测量结果显示了自旋玻璃动力学的有趣的随频率变化的磁行为特征。这种玻璃态的行为很可能归因于二镍(II)和二钴(II)前体的非晶态特征和/或中等至强的磁各向异性。

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