Thermal and transport properties of La2–xNdxMo2O9
来源期刊:JOURNAL OF RARE EARTHS2016年第10期
论文作者:闫柏军 任志华 侯新梅
文章页码:1024 - 1031
摘 要:Single-phase La2–xNdxMo2O9(0≤x≤1.8) compounds were prepared using solid-state reaction technique. Their structural and thermal p roperties were characterized by room and high temperatures X-ray diffraction(XRD), thermo gravimetric analysis-differential scanningcalorimetry(TG-DSC), and high temperature Raman spectra. The transport properties were investigated using D.C. four-probe technique and Hebb-Wagner polarization method. The substitution limit of Nb3+ in La2–xNdxMo2O9 was determined to be in the range of 1.8<x<1.9, and the cubic lattice parameter of La2–xNdxMo2O9 decreased linearly with the increasing of x. When the Nb3+ substitution content x was larger than 0.6, the α/β phase transition could be depressed to such a great degree that the phase transition thermal enthalpy was not detected by DSC. The temperature dependence of electrical conductivities for La1.4NdxMo2O9 below 873 K and that for LaNdMo2O9 below 923 K obeyed the Arrhenius law, while above 873 and 923 K Vogel-Tammann-Fulcher(VTF) model could describe the conduction behaviors satisfactorily. The transition of transport mechanism from Arrhenius to VTF was caused by the change of structure, which was supported by the high temperature XRD and Raman results. The ionic transport number of La1.4NdxMo2O9 in air was larger than 0.99 at 1073 K, and with the increasing of temperature it was close to 0.98 at 1173 K. In view of the phase transition, thermal expansion and conductivity properties, La1.4NdxMo2O9 should be a promising electrolyte material in La2–xNdxMo2O9 series.
闫柏军1,任志华1,2,侯新梅1
1. Department of Physical Chemistry of Metallurgy, University of Science and Technology Beijing2. School of Chemical Engineering,Qingdao University of Science and Technology
摘 要:Single-phase La2–xNdxMo2O9(0≤x≤1.8) compounds were prepared using solid-state reaction technique. Their structural and thermal p roperties were characterized by room and high temperatures X-ray diffraction(XRD), thermo gravimetric analysis-differential scanningcalorimetry(TG-DSC), and high temperature Raman spectra. The transport properties were investigated using D.C. four-probe technique and Hebb-Wagner polarization method. The substitution limit of Nb3+ in La2–xNdxMo2O9 was determined to be in the range of 1.8<x<1.9, and the cubic lattice parameter of La2–xNdxMo2O9 decreased linearly with the increasing of x. When the Nb3+ substitution content x was larger than 0.6, the α/β phase transition could be depressed to such a great degree that the phase transition thermal enthalpy was not detected by DSC. The temperature dependence of electrical conductivities for La1.4NdxMo2O9 below 873 K and that for LaNdMo2O9 below 923 K obeyed the Arrhenius law, while above 873 and 923 K Vogel-Tammann-Fulcher(VTF) model could describe the conduction behaviors satisfactorily. The transition of transport mechanism from Arrhenius to VTF was caused by the change of structure, which was supported by the high temperature XRD and Raman results. The ionic transport number of La1.4NdxMo2O9 in air was larger than 0.99 at 1073 K, and with the increasing of temperature it was close to 0.98 at 1173 K. In view of the phase transition, thermal expansion and conductivity properties, La1.4NdxMo2O9 should be a promising electrolyte material in La2–xNdxMo2O9 series.
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