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Synthesis and Magnetic Properties of the KCu(IO3)3 Compound with [CuO5] Chains.
Mitoudi-Vagourdi, Eleni; Rienmüller, Julia; Lemmens, Peter; Gnezdilov, Vladimir; Kremer, Reinhard K; Johnsson, Mats.
Afiliação
  • Mitoudi-Vagourdi E; Department of Materials and Environmental Chemistry, Stockholm University, SE-106 91 Stockholm, Sweden.
  • Rienmüller J; Department of Materials and Environmental Chemistry, Stockholm University, SE-106 91 Stockholm, Sweden.
  • Lemmens P; Institute for Condensed Matter Physics and Laboratory of Emerging Nanometrology LENA, TU Braunschweig, D-38106 Braunschweig, Germany.
  • Gnezdilov V; Institute for Condensed Matter Physics and Laboratory of Emerging Nanometrology LENA, TU Braunschweig, D-38106 Braunschweig, Germany.
  • Kremer RK; B. Verkin Institute for Low Temperature Physics and Engineering, NASU, 61103 Kharkov, Ukraine.
  • Johnsson M; Max Planck Institute for Solid State Research, Heisenbergstrasse 1, D-70569 Stuttgart, Germany.
ACS Omega ; 4(12): 15168-15174, 2019 Sep 17.
Article em En | MEDLINE | ID: mdl-31552362
ABSTRACT
The new quaternary iodate KCu(IO3)3 has been prepared by hydrothermal synthesis. KCu(IO3)3 crystallizes in the monoclinic space group P21/n with unit cell parameters a = 9.8143(4) Å, b = 8.2265(4) Å, c = 10.8584(5) Å, ß = 91.077(2)°, and z = 4. The crystals are light blue and translucent. There are three main building units making up the crystal structure [KO10] irregular polyhedra, [CuO6] distorted octahedra, and [IO3] trigonal pyramids. The Jahn-Teller elongated [CuO6] octahedra connect to each other via corner sharing to form [CuO5]∞ 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 [IO3E], 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 T C = 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 S = 1/2 antiferromagnetic Heisenberg chain with a nearest-neighbor spin exchange of ∼8.9 K.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: ACS Omega Ano de publicação: 2019 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: ACS Omega Ano de publicação: 2019 Tipo de documento: Article