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Jahn-Teller 畸变框架和 Rb-Mn-P-O 体系中的磁有序。

Jahn-Teller distorted frameworks and magnetic order in the Rb-Mn-P-O system.

机构信息

School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, UK.

出版信息

Inorg Chem. 2010 Feb 1;49(3):934-42. doi: 10.1021/ic901668u.

DOI:10.1021/ic901668u
PMID:20041645
Abstract

Two previously uncharacterized members of the Rb-Mn-P-O system, RbMnP(2)O(7) and beta-RbMnHP(3)O(10), have been synthesized using a phosphoric acid flux synthetic route and their crystal and magnetic structures determined using neutron powder diffraction. The crystal structure of RbMnP(2)O(7) (space group P2(1)/c, a = 7.3673(2) A, b = 9.6783(2) A, c = 8.6467(2) A, and beta = 105.487(1) degrees) was found to be isostructural with RbFeP(2)O(7). The polymorph beta-RbMnHP(3)O(10) was also isolated as a single phase and found to crystallize in the space group C2 (a = 12.2066(5) A, b = 8.5243(3) A, c = 8.8530(4) A, beta = 107.233(2) degrees). Both structures consist of frameworks of corner-sharing MnO(6) octahedra linked together by condensed phosphate anions, with Rb(+) cations located in the intersecting channels. In both cases the Mn(3+) octahedra exhibit unusual Jahn-Teller distortions indicative of a plasticity effect driven by the steric requirements of the condensed phosphate anions, and this causes a strong violet coloration similar to that observed in the manganese violet pigment; the structure of this has yet to be determined. Magnetic susceptibility measurements show that both RbMnP(2)O(7) (T(N) = 20 K) and beta-RbMnHP(3)O(10) (T(N) = 10 K) undergo a phase transition at low temperatures to an antiferromagnetically ordered state. Low-temperature neutron powder diffraction studies show that the magnetic ground states of each of these materials involve both ferromagnetic and antiferromagnetic super-superexchange interactions between orbitally ordered Mn(3+), which are mediated by PO(4) tetrahedra. These interactions are compared and discussed.

摘要

两个以前未被描述的 Rb-Mn-P-O 体系成员,RbMnP(2)O(7) 和β-RbMnHP(3)O(10),已经通过磷酸熔盐法合成,并通过中子粉末衍射确定了它们的晶体和磁性结构。RbMnP(2)O(7)(空间群 P2(1)/c,a = 7.3673(2) A,b = 9.6783(2) A,c = 8.6467(2) A,β = 105.487(1)°)的晶体结构被发现与 RbFeP(2)O(7) 同构。β-RbMnHP(3)O(10) 也被分离为单相,并被发现结晶在空间群 C2 中(a = 12.2066(5) A,b = 8.5243(3) A,c = 8.8530(4) A,β = 107.233(2)°)。这两个结构都由 MnO(6) 八面体通过缩合的磷酸盐阴离子连接而成,Rb(+) 阳离子位于交叉通道中。在这两种情况下,Mn(3+) 八面体都表现出不寻常的 Jahn-Teller 畸变,表明这是由缩合磷酸盐阴离子的空间要求驱动的塑性效应,这导致了强烈的紫色着色,类似于在锰紫颜料中观察到的;该结构尚未确定。磁化率测量表明,RbMnP(2)O(7)(T(N) = 20 K)和β-RbMnHP(3)O(10)(T(N) = 10 K)都在低温下经历了向反铁磁有序态的相变。低温中子粉末衍射研究表明,这些材料的磁基态都涉及轨道有序 Mn(3+) 之间的铁磁和反铁磁超交换相互作用,这些相互作用是由 PO(4) 四面体介导的。这些相互作用进行了比较和讨论。

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