Mitoudi-Vagourdi Eleni, Papawassiliou Wassilios, Müllner Silvia, Jaworski Aleksander, Pell Andrew J, Lemmens Peter, Kremer Reinhard K, Johnsson Mats
Department of Materials and Environmental Chemistry , Stockholm University , SE-106 91 Stockholm , Sweden.
Institute for Physics of Condensed Matter , TU Braunschweig , D-38106 Braunschweig , Germany.
Inorg Chem. 2018 Apr 16;57(8):4640-4648. doi: 10.1021/acs.inorgchem.8b00372. Epub 2018 Apr 3.
Single crystals of the new compound Cu(SeO)F were successfully synthesized via a hydrothermal method, and the crystal structure was determined from single-crystal X-ray diffraction data. The compound crystallizes in the orthorhombic space group Pnma with the unit cell parameters a = 7.066(4) Å, b = 9.590(4) Å, and c = 5.563(3) Å. Cu(SeO)F is isostructural with the previously described compounds CoTeOF and CoSeOF. The crystal structure comprises a framework of corner- and edge-sharing distorted [CuOF] octahedra, within which [SeO] trigonal pyramids are present in voids and are connected to [CuOF] octahedra by corner sharing. The presence of a single local environment in both the F and Se solid-state MAS NMR spectra supports the hypothesis that O and F do not mix at the same crystallographic positions. Also the specific phonon modes observed with Raman scattering support the coordination around the cations. At high temperatures the magnetic susceptibility follows the Curie-Weiss law with Curie temperature of Θ = -173(2) K and an effective magnetic moment of μ ∼ 2.2 μ. Antiferromagnetic ordering below ∼44 K is indicated by a peak in the magnetic susceptibility. A second though smaller peak at ∼16 K is tentatively ascribed to a magnetic reorientation transition. Both transitions are also confirmed by heat capacity measurements. Raman scattering experiments propose a structural phase instability in the temperature range 6-50 K based on phonon anomalies. Further changes in the Raman shift of modes at ∼46 K and ∼16 K arise from transitions of the magnetic lattice in accordance with the susceptibility and heat capacity measurements.
通过水热法成功合成了新化合物Cu(SeO)F的单晶,并根据单晶X射线衍射数据确定了其晶体结构。该化合物结晶于正交晶系空间群Pnma中,晶胞参数为a = 7.066(4) Å,b = 9.590(4) Å,c = 5.563(3) Å。Cu(SeO)F与先前描述的化合物CoTeOF和CoSeOF同构。晶体结构由角共享和边共享的扭曲[CuOF]八面体框架组成,其中[SeO]三角锥存在于空隙中,并通过角共享与[CuOF]八面体相连。F和Se的固态MAS NMR谱中单一局部环境的存在支持了O和F不在相同晶体学位置混合的假设。拉曼散射观察到的特定声子模式也支持阳离子周围的配位情况。在高温下,磁化率遵循居里-外斯定律,居里温度为Θ = -173(2) K,有效磁矩为μ ∼ 2.2 μ。低于约44 K时的反铁磁有序由磁化率峰值表示。在约16 K处的第二个较小峰值暂归因于磁取向转变。这两个转变也通过热容测量得到证实。拉曼散射实验基于声子异常提出在6 - 50 K温度范围内存在结构相不稳定性。根据磁化率和热容测量,在约46 K和约16 K处模式的拉曼位移的进一步变化源于磁晶格的转变。