Department of Chemistry, Shippensburg University, Shippensburg, Pennsylvania 17257-2200, United States.
Inorg Chem. 2011 Nov 21;50(22):11348-52. doi: 10.1021/ic2008792. Epub 2011 Oct 21.
The magnetic behavior of the pentanuclear complex of formula Mn(II)(O(2)CCH(3))(2)12-MC(Mn(III)(N)shi)-4(6), 1, was investigated using magnetization and magnetic susceptibility measurements both in the solid state and in solution. Complex 1 has a nearly planar structure, made of a central Mn(II) ion surrounded by four peripheral Mn(III) ions. Solid state variable-field dc magnetic susceptibility experiments demonstrate that 1 possesses a low value for the total spin in the ground state; fitting appropriate expressions to the data results in antiferromangetic coupling both between the peripheral Mn(III) ions (J = -6.3 cm(-1)) and between the central Mn(II) ion and the Mn(III) ones (J' = -4.2 cm(-1)). In order to obtain a reasonable fit, a relatively large single ion magnetic anisotropy (D) value of 1 cm(-1) was necessary for the central Mn(II) ion. The single crystal magnetization measurements using a microsquid array display a very slight opening of the hysteresis loop but only at a very low temperature (0.04 K), which is in line with the ac susceptibility data where a slow relaxation of the magnetization occurs just around 2 K. In frozen solution, complex 1 displays a frequency dependent ac magnetic susceptibility signal with an energy barrier to magnetization reorientation (E) and relaxation time at an infinite temperature (τ(o)) of 14.7 cm(-1) and 1.4 × 10(-7) s, respectively, demonstrating the single molecule magnetic behavior in solution.
通过对固态和溶液状态下的磁化强度和磁化率进行测量,研究了分子式为Mn(II)(O(2)CCH(3))(2)12-MC(Mn(III)(N)shi)-4(6)的五核配合物1的磁行为。配合物1具有近乎平面的结构,由一个中心Mn(II)离子和四个外围Mn(III)离子组成。固态可变场直流磁化率实验表明,1在基态的总自旋值较低;将合适的表达式拟合到数据中,结果表明外围Mn(III)离子之间(J = -6.3 cm(-1))以及中心Mn(II)离子与Mn(III)离子之间(J' = -4.2 cm(-1))存在反铁磁耦合。为了获得合理的拟合,中心Mn(II)离子需要一个相对较大的单离子磁各向异性(D)值,为1 cm(-1)。使用微量子阵列进行的单晶磁化强度测量显示,磁滞回线仅有非常轻微的开口,但仅在非常低的温度(0.04 K)下出现,这与交流磁化率数据一致,在交流磁化率数据中,磁化强度的缓慢弛豫恰好在2 K左右发生。在冷冻溶液中,配合物1显示出频率依赖的交流磁化率信号,其磁化重新取向的能垒(E)和无限温度下的弛豫时间(τ(o))分别为14.7 cm(-1)和1.4×10(-7) s,证明了其在溶液中的单分子磁行为。