Research Institute for Ubiquitous Energy Devices, National Institute of Advanced Industrial Science and Technology, Midorigaoka 1-8-31, Ikeda, Osaka 563-8577, Japan.
Inorg Chem. 2012 Aug 20;51(16):8729-38. doi: 10.1021/ic300374w. Epub 2012 Aug 2.
The new compound LiNaCo[PO(4)]F was synthesized by a solid state reaction route, and its crystal structure was determined by single-crystal X-ray diffraction measurements. The magnetic properties of LiNaCo[PO(4)]F were characterized by magnetic susceptibility, specific heat, and neutron powder diffraction measurements and also by density functional calculations. LiNaCo[PO(4)]F crystallizes with orthorhombic symmetry, space group Pnma, with a = 10.9334(6), b = 6.2934(11), c = 11.3556(10) Å, and Z = 8. The structure consists of edge-sharing CoO(4)F(2) octahedra forming CoFO(3) chains running along the b axis. These chains are interlinked by PO(4) tetrahedra forming a three-dimensional framework with the tunnels and the cavities filled by the well-ordered sodium and lithium atoms, respectively. The magnetic susceptibility follows the Curie-Weiss behavior above 60 K with θ = -21 K. The specific heat and magnetization measurements show that LiNaCo[PO(4)]F undergoes a three-dimensional magnetic ordering at T(mag) = 10.2(5) K. The neutron powder diffraction measurements at 3 K show that the spins in each CoFO(3) chain along the b-direction are ferromagnetically coupled, while these FM chains are antiferromagnetically coupled along the a-direction but have a noncollinear arrangement along the c-direction. The noncollinear spin arrangement implies the presence of spin conflict along the c-direction. The observed magnetic structures are well explained by the spin exchange constants determined from density functional calculations.
新的化合物 LiNaCo[PO(4)]F 是通过固相反应路线合成的,并通过单晶 X 射线衍射测量确定了其晶体结构。通过磁化率、比热和中子粉末衍射测量以及密度泛函计算研究了 LiNaCo[PO(4)]F 的磁性。LiNaCo[PO(4)]F 结晶为正交晶系,空间群为 Pnma,晶胞参数分别为 a = 10.9334(6) Å、b = 6.2934(11) Å、c = 11.3556(10) Å,Z = 8。结构由共边的 CoO(4)F(2)八面体组成,形成 CoFO(3)链,沿 b 轴排列。这些链由 PO(4)四面体相互连接,形成一个三维骨架,隧道和空腔分别由有序的钠离子和锂离子填充。磁化率在 60 K 以上遵循居里-外斯行为,θ = -21 K。比热和磁化率测量表明,LiNaCo[PO(4)]F 在 T(mag) = 10.2(5) K 时经历三维磁有序。3 K 下的中子粉末衍射测量表明,b 方向上每个 CoFO(3)链中的自旋呈铁磁耦合,而这些 FM 链沿 a 方向反铁磁耦合,但沿 c 方向呈非共线排列。非共线自旋排列意味着沿 c 方向存在自旋冲突。观察到的磁结构可以通过密度泛函计算确定的自旋交换常数很好地解释。