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展现单分子磁体行为的新型Mn₃Ln₄簇合物家族。

A family of novel Mn₃Ln₄ clusters displaying single-molecule magnet behavior.

作者信息

Chen Hui, Ma Cheng-Bing, Hu Ming-Qiang, Wen Hui-Min, Chen Chang-Neng

机构信息

State Key Laboratory of Structural Chemistry, Fujian Institute of Research on the Structure of Matter, The Chinese Academy of Sciences, Fuzhou, Fujian 350002, China.

出版信息

Dalton Trans. 2014 Nov 28;43(44):16737-44. doi: 10.1039/c4dt01816h.

Abstract

Using 3-methyloxysalicylaldoxime (mosaoH2) and N-methyl diethanolamine (N-mdeaH2) as coligands, a family of heptanuclear Mn/Ln heterometallic compounds [Mn(II)Mn(III)2Ln(III)4(mosao)2(mosaoH)4(piv)4(N-mdea)4]·xMeCN [Ln = Dy(1), Tb(2) and Y(3), pivH = pivalic acid] have been prepared. The crystal structures of 1-3 were obtained, and their core consists of two Mn(III)Ln2(μ3-OR)2 (RO(2-) = N-mdea(2-)) triangles linked to a central Mn(II) atom. A dc magnetic susceptibility study reveals that single-ion effects of the Ln ions are dominant in compounds 1 and 2. As for compound 3, which contains diamagnetic Y ions, the magnetic interactions between Mn ions via oximate NO bridges are revealed to be ferromagnetic. Fitting of the χ(m)T vs. T data gives g = 1.96 and J = 1.12 cm(-1), affording a S = 13/2 ground state. All of the three compounds exhibit frequency-dependent out-of-phase ac susceptibility signals indicative of slow magnetization relaxation and potential SMM behavior. Among them, 1 and 3 display the out-of-phase χ"(m) peak maximum above 2.0 K. Fitting of the ac susceptibility data to the Arrhenius law gives an energy barrier U(eff) = 9.27/13.83 K for 1 and 3, respectively.

摘要

以3-甲氧基水杨醛肟(mosaoH2)和N-甲基二乙醇胺(N-mdeaH2)作为共配体,制备了一系列七核Mn/Ln异金属化合物[Mn(II)Mn(III)2Ln(III)4(mosao)2(mosaoH)4(piv)4(N-mdea)4]·xMeCN [Ln = Dy(1)、Tb(2) 和 Y(3),pivH = 新戊酸]。获得了1-3的晶体结构,其核心由两个与中心Mn(II)原子相连的Mn(III)Ln2(μ3-OR)2(RO(2-) = N-mdea(2-))三角形组成。直流磁化率研究表明,Ln离子的单离子效应在化合物1和2中占主导地位。至于含有抗磁性Y离子的化合物3,通过肟基NO桥的Mn离子之间的磁相互作用被揭示为铁磁性。χ(m)T对T数据的拟合给出g = 1.96和J = 1.12 cm(-1),得到S = 13/2的基态。这三种化合物均表现出频率依赖的异相交流磁化率信号,表明存在缓慢的磁化弛豫和潜在的单分子磁体行为。其中,1和3在2.0 K以上显示出异相χ"(m)峰值最大值。将交流磁化率数据拟合到阿仑尼乌斯定律,分别得到1和3的能垒U(eff) = 9.27/13.83 K。

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