M. V. Lomonosov Moscow State University, Moscow 119991, Russia.
Inorg Chem. 2013 Feb 4;52(3):1538-43. doi: 10.1021/ic302333e. Epub 2013 Jan 18.
Mixed potassium-manganese vanadate-carbonate, K(2)Mn(3)(VO(4))(2)(CO(3)), represents a novel structure type; it has been synthesized hydrothermally from the system MnCl(2)-K(2)CO(3)-V(2)O(5)-H(2)O. Its hexagonal crystal structure was determined by single-crystal X-ray diffraction with a = 5.201(1) Å, c = 22.406(3) Å, space group P6(3)/m, Z = 2, ρ(c) = 3.371 g/cm(3), and R = 0.022. The layered structure of the compound can be described as a combination of honeycomb-type modules of [MnO(6)] octahedra and [VO(4)] tetrahedra, alternating in the [001] direction with layers of [MnCO(3)] built by [MnO(5)] trigonal bipyramids and [CO(3)] planar triangles, sharing oxygen vertices. The K(+) ions are placed along channels of the framework, elongated in the [100], [010], and [110] directions. The title compound exhibits rich physical properties reflected in a phase transition of presumably Jahn-Teller origin at T(3) = 80-100 K as well as two successive magnetic phase transitions at T(2) = 3 K and T(1) = 2 K into a weakly ferromagnetic ground state, as evidenced in magnetization, specific heat, and X-band electron spin resonance measurements. A negative Weiss temperature Θ = -114 K and strongly reduced effective magnetic moment μ(eff)(2) ~ 70 μ(B)(2) per formula unit suggest that antiferromagnetic exchange interactions dominate in the system. Divalent manganese is present in a high-spin state, S = 5/2, in the octahedral environment and a low-spin state, S = ½, in the trigonal-bipyramidal coordination.
钾锰钒酸盐-碳酸盐,K(2)Mn(3)(VO(4))(2)(CO(3)),代表了一种新的结构类型;它是通过在 MnCl(2)-K(2)CO(3)-V(2)O(5)-H(2)O 体系中进行水热合成得到的。它的六方晶体结构通过单晶 X 射线衍射确定,晶胞参数为 a = 5.201(1) Å,c = 22.406(3) Å,空间群 P6(3)/m,Z = 2,ρ(c) = 3.371 g/cm(3),R = 0.022。化合物的层状结构可以描述为 [MnO(6)]八面体和 [VO(4)]四面体的蜂窝状模块的组合,在 [001]方向上交替排列,由 [MnO(5)]三角双锥和 [CO(3)]平面三角形构成的 [MnCO(3)]层堆积而成,氧原子作为顶点共享。K(+)离子位于框架的通道中,沿 [100]、[010]和 [110]方向拉长。标题化合物表现出丰富的物理性质,反映在 T(3) = 80-100 K 处可能为 Jahn-Teller 起源的相变以及在 T(2) = 3 K 和 T(1) = 2 K 处进入弱铁磁基态的两个连续磁相变,这在磁化率、比热和 X 波段电子自旋共振测量中得到了证明。负 Weiss 温度 Θ = -114 K 和强烈降低的有效磁矩 μ(eff)(2)~70 μ(B)(2)每分子式单位表明,反铁磁交换相互作用在该体系中占主导地位。二价锰在八面体环境中处于高自旋态 S = 5/2,在三角双锥配位中处于低自旋态 S = 1/2。