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Effect of manganese doping on vibrational and physical properties of ZrTe3O8.

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Title: Effect of manganese doping on vibrational and physical properties of ZrTe3O8.
Authors: Koubaa, M.1, Karray, R.1, Dhifallah, N.2, Kabadou, A.1 ahlemkabadou@yahoo.fr, Bsais, L.3
Source: Journal of Alloys & Compounds. Jun2017, Vol. 709, p808-818. 11p.
Subjects: Vibration (Mechanics), Zirconium compounds, Solid state chemistry, Doping agents (Chemistry), Crystal structure
Abstract: The powder sample of xMnO 2 –(1−x) ZrTe 3 O 8 (x = 7%) was prepared by the conventional solid state reaction method. X-ray diffraction showed that the compound crystallized at room temperature in the cubic fluorite structure (in a cubic unit-cell Ia 3 ¯ as MTe 3 O 8 -type framework) with lattice parameter a = 11.3298(2) Ǻ. The structure was built up of TeO 4 E (E = Electronic lone pair of Te(IV)) disphnoids and regular ZrO 6 octahedra. The crystal structure cohesion was ensured via Te O(2) Zr and Te O(1) Te bridges. The Raman spectrum was dominated by a stronger band at 858 cm −1 , characteristic of Te O(2) Zr bridges asymmetric stretching vibration. Thus, the Te O(2) and Zr(Mn) O(2) bonds are chemically inequivalent and then the Te O(2) Zr bridges are chemically asymmetric. Magnetization measurements versus temperature in an applied magnetic field of 0.05 T were determined. The doping of Zr by Mn induces a ferro-paramagnetic transition at T = 18.5 K. The complex impedance of the xMnO 2 -(1−x) ZrTe 3 O 8 (x = 7%) ceramics has been investigated in the temperature range 293–843 K and in the frequency range 100 Hz–1 MHz. Dielectric data were analyzed using complex permittivity (ε′), (ε″) and tan (δ) for the sample at various temperatures. The conductivity follows the Arrhenius relation. [ABSTRACT FROM AUTHOR]
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Database: Engineering Source
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Abstract:The powder sample of xMnO 2 –(1−x) ZrTe 3 O 8 (x = 7%) was prepared by the conventional solid state reaction method. X-ray diffraction showed that the compound crystallized at room temperature in the cubic fluorite structure (in a cubic unit-cell Ia 3 ¯ as MTe 3 O 8 -type framework) with lattice parameter a = 11.3298(2) Ǻ. The structure was built up of TeO 4 E (E = Electronic lone pair of Te(IV)) disphnoids and regular ZrO 6 octahedra. The crystal structure cohesion was ensured via Te O(2) Zr and Te O(1) Te bridges. The Raman spectrum was dominated by a stronger band at 858 cm −1 , characteristic of Te O(2) Zr bridges asymmetric stretching vibration. Thus, the Te O(2) and Zr(Mn) O(2) bonds are chemically inequivalent and then the Te O(2) Zr bridges are chemically asymmetric. Magnetization measurements versus temperature in an applied magnetic field of 0.05 T were determined. The doping of Zr by Mn induces a ferro-paramagnetic transition at T = 18.5 K. The complex impedance of the xMnO 2 -(1−x) ZrTe 3 O 8 (x = 7%) ceramics has been investigated in the temperature range 293–843 K and in the frequency range 100 Hz–1 MHz. Dielectric data were analyzed using complex permittivity (ε′), (ε″) and tan (δ) for the sample at various temperatures. The conductivity follows the Arrhenius relation. [ABSTRACT FROM AUTHOR]
ISSN:09258388
DOI:10.1016/j.jallcom.2017.03.053