School of Chemistry, Monash University, Building 23, Clayton, Victoria 3800, Australia.
Inorg Chem. 2013 Jun 17;52(12):7183-92. doi: 10.1021/ic400789k. Epub 2013 May 29.
Three new heterometallic complexes with formulas of [Dy(III)2Co(III)2(OMe)2(teaH)2(acac)4(NO3)2] (1), [Dy(III)2Co(III)2(OH)2(teaH)2(acac)4(NO3)2]·4H2O (2), and [Dy(III)2Co(III)2(OMe)2(mdea)2(acac)4(NO3)2] (3) were characterized by single-crystal X-ray diffraction and by dc and ac magnetic susceptibility measurements. All three complexes have an identical "butterfly"-type metallic core that consists of two Dy(III) ions occupying the "body" position and two diamagnetic low-spin Co(III) ions occupying the outer "wing-tips". Each complex displays single-molecule magnet (SMM) behavior in zero applied magnetic field, with thermally activated anisotropy barriers of 27, 28, and 38 K above 7.5 K for 1-3, respectively, as well as observing a temperature-independent mechanism of relaxation below 5 K for 1 and 2 and at 3 K for 3, indicating fast quantum tunneling of magnetization (QTM). A second, faster thermally activated relaxation mechanism may also be active under a zero applied dc field as derived from the Cole-Cole data. Interestingly, these complexes demonstrate further relaxation modes that are strongly dependent upon the application of a static dc magnetic field. Dilution experiments that were performed on 1, in the {Y(III)2Co(III)2} diamagnetic analog, show that the slow magnetic relaxation is of a single-ion origin, but it was found that the neighboring ion also plays an important role in the overall relaxation dynamics.
三个新的异金属配合物的公式为[Dy(III)2Co(III)2(OMe)2(teaH)2(acac)4(NO3)2](1)、[Dy(III)2Co(III)2(OH)2(teaH)2(acac)4(NO3)2]·4H2O(2)和[Dy(III)2Co(III)2(OMe)2(mdea)2(acac)4(NO3)2](3),通过单晶 X 射线衍射和直流和交流磁化率测量进行了表征。这三个配合物都有一个相同的“蝴蝶”型金属核,由两个占据“体”位置的 Dy(III)离子和两个占据外“翼尖”的顺磁性低自旋 Co(III)离子组成。每个配合物在零外磁场下表现出单分子磁体(SMM)行为,在 7.5 K 以上,1-3 的热激活各向异性势垒分别为 27、28 和 38 K,以及在 1 和 2 低于 5 K 下观察到与温度无关的弛豫机制,表明磁化的快速量子隧道(QTM)。第二个更快的热激活弛豫机制也可能在零直流外场下作为 Cole-Cole 数据的推导而活跃。有趣的是,这些配合物表现出进一步的弛豫模式,这些模式强烈依赖于静态直流磁场的应用。在 1 中进行的稀释实验,在{Y(III)2Co(III)2}抗磁性类似物中,表明缓慢的磁弛豫是单离子起源的,但发现相邻离子在整体弛豫动力学中也起着重要作用。