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Thermoelectric Properties of Bi2Te3: CuI and the Effect of Its Doping with Pb Atoms

机译:Bi2Te3:CuI的热电性质及其掺杂Pb原子的影响

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摘要

In order to understand the effect of Pb-CuI co-doping on the thermoelectric performance of Bi2Te3, n-type Bi2Te3 co-doped with x at % CuI and 1/2x at % Pb (x = 0, 0.01, 0.03, 0.05, 0.07, and 0.10) were prepared via high temperature solid state reaction and consolidated using spark plasma sintering. Electron and thermal transport properties, i.e., electrical conductivity, carrier concentration, Hall mobility, Seebeck coefficient, and thermal conductivity, of CuI-Pb co-doped Bi2Te3 were measured in the temperature range from 300 K to 523 K, and compared to corresponding x% of CuI-doped Bi2Te3 and undoped Bi2Te3. The addition of a small amount of Pb significantly decreased the carrier concentration, which could be attributed to the holes from Pb atoms, thus the CuI-Pb co-doped samples show a lower electrical conductivity and a higher Seebeck coefficient when compared to CuI-doped samples with similar x values. The incorporation of Pb into CuI-doped Bi2Te3 rarely changed the power factor because of the trade-off relationship between the electrical conductivity and the Seebeck coefficient. The total thermal conductivity(κtot) of co-doped samples (κtot ~ 1.4 W/m∙K at 300 K) is slightly lower than that of 1% CuI-doped Bi2Te3 (κtot ~ 1.5 W/m∙K at 300 K) and undoped Bi2Te3tot ~ 1.6 W/m∙K at 300 K) due to the alloy scattering. The 1% CuI-Pb co-doped Bi2Te3 sample shows the highest ZT value of 0.96 at 370 K. All data on electrical and thermal transport properties suggest that the thermoelectric properties of Bi2Te3 and its operating temperature can be controlled by co-doping.
机译:为了了解Pb-CuI共掺杂对Bi2Te3热电性能的影响,n型Bi2Te3共掺杂有x含量为CuI的x和1 / 2x含量为Pb的x(x = 0、0.01、0.03、0.05,通过高温固态反应制备0.07和0.10),并使用火花等离子体烧结进行固结。在300 K至523 K的温度范围内测量了CuI-Pb共掺杂Bi2Te3的电子和热传输性质,即电导率,载流子浓度,霍尔迁移率,塞贝克系数和热导率,并与相应的x进行了比较。 CuI掺杂的Bi2Te3和未掺杂的Bi2Te3的百分比。少量Pb的添加显着降低了载流子浓度,这可能归因于Pb原子的空穴,因此与CuI掺杂相比,CuI-Pb共掺杂样品显示出较低的电导率和较高的塞贝克系数x值相似的样本。由于电导率和塞贝克系数之间存在折衷关系,因此将Pb掺入CuI掺杂的Bi2Te3中几乎不会改变功率因数。共掺杂样品的总热导率(κtot)(在300 K时为κtot〜1.4 W / m∙K)略低于1%掺杂CuI的Bi2Te3(κ 〜1.5 W / m∙K在300 K时)和未掺杂的Bi 2 Te 3 (在300 K时κ tot 〜1.6 W / m∙K)对合金的散射。 1%CuI-Pb共掺杂的Bi 2 Te 3 样品在370 K时显示出最高的ZT值为0.96。有关电学和热学传输性质的所有数据表明, Bi 2 Te 3 的热电性质及其工作温度可以通过共掺杂来控制。

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