Jovaní Marc, Beltrán-Mir Héctor, Cordoncillo Eloisa, West Anthony R
Departamento de Química Inorgánica y Orgánica, Universidad Jaume I , Avenida Sos Baynat s/n, Castellón 12071, Spain.
Department of Materials Science & Engineering, University of Sheffield , Mappin Street, Sheffield S1 3JD, U.K.
Inorg Chem. 2017 Jun 19;56(12):7081-7088. doi: 10.1021/acs.inorgchem.7b00673. Epub 2017 May 26.
Cubic, fluorite-structured solid solutions ZrYO (YSZ; x = 0.4-0.7) were prepared by sol-gel synthesis. Impedance measurements on pellets of 85% approximate density sintered at 1300 °C for 24 h showed strong evidence of oxide ion conduction with an inclined Warburg spike at low frequencies and capacitance values of ∼10 F cm at 40 Hz. Arrhenius plots of total pellet conductivities were linear with activation energies of 1.4-1.56 eV. The conductivity decreased with x and was 2-4 orders of magnitude lower than that with optimized YSZ, x = 0.08. When the atmosphere was changed from N to O during impedance measurements, two reversible effects were seen: the Warburg spike contracted greatly, and the sample resistance decreased. These effects were more noticeable at higher x and are attributed to the introduction of p-type electronic conduction, in parallel with the preexisting oxide ion conduction. A similar reversible result was observed upon application of a direct-current (dc) bias during impedance measurements. When either pO is increased or a dc bias is applied, hole creation is believed to arise by the ionization of underbonded oxide ions situated near the Y dopant ions. The ionized electrons are trapped at surface oxygen species, and the holes that are left on oxygen are responsible for p-type conduction. The electrolytic domain of x = 0.4-0.7 extends up to approximately 10 atm of O before p-type conduction is observed. The upper pO limit of the electrolytic domain of x = 0.08 is not known but is likely to be close to or slightly above 1 atm of O.
通过溶胶 - 凝胶合成法制备了立方萤石结构的固体溶液ZrYO(YSZ;x = 0.4 - 0.7)。对在1300℃烧结24小时、密度约为85%的颗粒进行阻抗测量,结果显示出强烈的氧离子传导证据,在低频下有倾斜的Warburg峰,且在40Hz时电容值约为10F/cm²。总颗粒电导率的阿伦尼乌斯曲线呈线性,活化能为1.4 - 1.56eV。电导率随x值降低,比优化后的YSZ(x = 0.08)低2 - 4个数量级。在阻抗测量期间,当气氛从N₂变为O₂时,观察到两种可逆效应:Warburg峰大幅收缩,样品电阻降低。这些效应在x值较高时更明显,这归因于与预先存在的氧离子传导并行引入的p型电子传导。在阻抗测量期间施加直流(dc)偏压时,观察到类似的可逆结果。当pO₂增加或施加直流偏压时,据信空穴的产生是由于位于Y掺杂离子附近的欠键合氧离子的电离。电离的电子被捕获在表面氧物种上,留在氧上的空穴负责p型传导。在观察到p型传导之前,x = 0.4 - 0.7的电解区域延伸至约10atm的O₂。x = 0.08的电解区域的pO₂上限未知,但可能接近或略高于1atm的O₂。