首页> 外文期刊>Solid state ionics >Seebeck coefficient and electrical conductivity of BSCF (Ba _(0.5)Sr _(0.5)Co _xFe _(1 - X)O _(3 - δ), 0 ≤ x ≤ 0.8) as a function of temperature and partial oxygen pressure
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Seebeck coefficient and electrical conductivity of BSCF (Ba _(0.5)Sr _(0.5)Co _xFe _(1 - X)O _(3 - δ), 0 ≤ x ≤ 0.8) as a function of temperature and partial oxygen pressure

机译:BSCF(Ba _(0.5)Sr _(0.5)Co _xFe _(1- X)O _(3-δ),0≤x≤0.8的塞贝克系数和电导率随温度和氧分压的函数

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The electrical conductivity and Seebeck coefficient of sintered BSCF ceramics (Ba _(0.5)Sr _(0.5)Co _xFe _(1 - x)O _(3 - δ), 0 ≤ x ≤ 0.8) were simultaneously measured as a function of pO _2 (10 ~(- 5) ≤ pO _2 ≤ 1 atm) at 500 °C, 700 °C and 900 °C. All samples exhibited a positive Seebeck coefficient over the range of pO _2 and temperature examined, which indicates the predominance of p-type conduction. In all cases, conductivity increased with increasing pO _2, ranging from a minimum of ~ 0.6 S/cm (x = 0, pO _2 = 10 ~(- 5) atm, T = 900 °C) to a maximum of ~ 36 S/cm (x = 0.8, pO _2 = 1 atm, and T = 900 °C). At low temperatures and high pO _2, conductivity was approximately proportional to pO _2 ~(1/4), which was attributed to the reduction of B-site cations from their tetravalent to trivalent state. At low pO _2 and high temperature, the conductivity exhibited positive deviations from the pO _2 ~(1/4) dependence. At 500 °C and x ≤ 0.6, the Seebeck coefficient (Q) decreased linearly with increasing log pO _2. At 700 and 900 °C, Q vs. log pO _2 curves exhibited maxima at 10 ~(- 3) < pO _2 < 10 ~(- 1) atm, and the maxima shifted to higher pO _2 as x increased. A simple p-type polaron hopping model, assuming negligible contribution from n-type or ionic carriers, was used to extract the carrier concentration of the x = 0.8 sample from the measured thermopower data. The calculated hole mobility for the x = 0.8 sample was less than 0.1 cm ~2/V-s, confirming a p-type polaron-hopping model. This analysis, as well as analysis of Jonker plots, suggested that hole mobility decreased with decreasing pO _2.
机译:同时测量了BSCF烧结陶瓷(Ba _(0.5)Sr _(0.5)Co _xFe _(1- x)O _(3-δ),0≤x≤0.8)的电导率和塞贝克系数。在500°C,700°C和900°C下pO _2(10〜(-5)≤pO _2≤1 atm)。所有样品在pO _2和检测温度范围内均表现出正Seebeck系数,这表明p型导电占主导地位。在所有情况下,电导率随pO _2的增加而增加,范围从最小〜0.6 S / cm(x = 0,pO _2 = 10〜(-5)atm,T = 900°C)到最大〜36 S / cm(x = 0.8,pO _2 = 1 atm,T = 900°C)。在低温和高pO _2下,电导率大约与pO _2〜(1/4)成正比,这归因于B位阳离子从其四价态还原为三价态。在低pO _2和高温下,电导率与pO _2〜(1/4)依赖性呈正偏差。在500°C和x≤0.6的情况下,塞贝克系数(Q)随log pO _2的增加而线性下降。在700和900°C下,Q与log pO _2曲线在10〜(-3)O _2 <10〜(-1)atm处显示最大值,并且随着x的增加,最大值移至更高的pO _2。假设n型或离子载流子的贡献可忽略不计,一个简单的p型极化子跳跃模型用于从测得的热功率数据中提取x = 0.8样品的载流子浓度。 x = 0.8样品的计算空穴迁移率小于0.1 cm〜2 / V-s,证实了p型极化子跳跃模型。该分析以及Jonker图的分析表明,空穴迁移率随pO _2的降低而降低。

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