Mitoudi-Vagourdi Eleni, Rienmüller Julia, Lemmens Peter, Gnezdilov Vladimir, Kremer Reinhard K, Johnsson Mats
Department of Materials and Environmental Chemistry, Stockholm University, SE-106 91 Stockholm, Sweden.
Institute for Condensed Matter Physics and Laboratory of Emerging Nanometrology LENA, TU Braunschweig, D-38106 Braunschweig, Germany.
ACS Omega. 2019 Aug 30;4(12):15168-15174. doi: 10.1021/acsomega.9b02064. eCollection 2019 Sep 17.
The new quaternary iodate KCu(IO) has been prepared by hydrothermal synthesis. KCu(IO) crystallizes in the monoclinic space group 2/ with unit cell parameters = 9.8143(4) Å, = 8.2265(4) Å, = 10.8584(5) Å, β = 91.077(2)°, and = 4. The crystals are light blue and translucent. There are three main building units making up the crystal structure: [KO] irregular polyhedra, [CuO] distorted octahedra, and [IO] trigonal pyramids. The Jahn-Teller elongated [CuO] octahedra connect to each other via corner sharing to form [CuO] zigzag chains along [010]; the other building blocks separate these chains. The Raman modes can be divided into four groups; the lower two groups into mainly lattice modes involving K and Cu displacements and the upper two groups into mainly bending and stretching modes of [IOE], where E represents a lone pair of electron. At low temperatures, the magnetic susceptibility is characterized by a broad maximum centered at ∼5.4 K, characteristic for antiferromagnetic short-range ordering. Long-range magnetic ordering at = 1.32 K is clearly evidenced by a sharp anomaly in the heat capacity. The magnetic susceptibility can be very well described by a spin = 1/2 antiferromagnetic Heisenberg chain with a nearest-neighbor spin exchange of ∼8.9 K.
新型四碘酸盐KCu(IO)已通过水热合成法制备出来。KCu(IO)以单斜空间群2/结晶,晶胞参数为 = 9.8143(4) Å, = 8.2265(4) Å, = 10.8584(5) Å,β = 91.077(2)°,且 = 4。晶体呈浅蓝色且半透明。有三种主要结构单元构成晶体结构:[KO]不规则多面体、[CuO]畸变八面体和[IO]三角锥。Jahn - Teller拉长的[CuO]八面体通过共角相连,沿着[010]方向形成[CuO]锯齿链;其他结构单元将这些链分隔开。拉曼模式可分为四组;较低的两组主要是涉及K和Cu位移的晶格模式,较高的两组主要是[IOE](其中E代表孤对电子)的弯曲和拉伸模式。在低温下,磁化率的特征是在约5.4 K处有一个宽峰,这是反铁磁短程有序的特征。在 = 1.32 K时的长程磁有序通过热容中的尖锐异常清晰地体现出来。磁化率可以用一个自旋 = 1/2的反铁磁海森堡链很好地描述,其最近邻自旋交换约为8.9 K。