G.A. Ahmed , A.M. Adam , Vyacheslav Khavrus , Silke Hampel , E.M.M. Ibrahim
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The PL spectra exhibit a strong peak at the wavelength 401 nm which is ascribed to a recombination of excitons and/or shallowly trapped electron–hole pairs. The thermoelectric properties are studied in the temperature range of 300–500 K and confirm the domination of p-type conduction in the whole temperature range. The electrical conductivity (<em>σ</em>) versus temperature showed thermally activated behavior as the charge carrier mobility is activated and the average carrier kinetic energy increases with temperature. Activation energy was obtained from the plots of Ln <em>σ</em> as a function of 1000/T. The recorded values were found at 62, 50,73 and 34 meV for x = 0, 0.04, 0.06 and 0.08, respectively. The Seebeck coefficients (<em>S</em>) of the synthesized nanostructures revealed a dominance of p-type conduction due to consistently positive S values. The S-T plots exhibit an initial increase in S with temperature at lower values (T < Tₛ). 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引用次数: 0
摘要
目前的工作研究了掺锑对水热法制造的碲化镉纳米结构的形态、光学行为和热电性能的影响。利用 X 射线衍射 (XRD) 和拉曼光谱技术进行的分析表明,存在立方相,这是碲化镉化合物的显著特征。扫描电子显微镜和高分辨率透射电子显微镜对样品的形态和内部结构进行了检测。光致发光光谱显示带隙能量约为 3.0 eV,高于块状样品的带隙能量。拉曼光谱显示出三个峰值,分别对应于 PbTe 的纵向光学(LO)声子模式和高次谐波多声子过程。聚光光谱在波长 401 nm 处显示出一个强峰值,这是由于激子和/或浅俘获电子-空穴对的重组所致。在 300-500 K 的温度范围内对热电性能进行了研究,结果证实在整个温度范围内 p 型传导占主导地位。电导率(σ)与温度的关系表现出热激活行为,因为电荷载流子迁移率被激活,平均载流子动能随温度升高而增加。活化能是从 Ln σ 与 1000/T 的函数关系图中获得的。在 x = 0、0.04、0.06 和 0.08 时,记录的值分别为 62、50、73 和 34 meV。合成纳米结构的塞贝克系数(S)显示,由于 S 值始终为正,因此 p 型传导占主导地位。S-T 图显示,在较低值 (T < Tₛ)时,S 值最初随温度升高而增加。然而,在特定温度(Tₛ)下会发生转变,其标志是 S 值从正值阶跃变为负值,随后随着温度的进一步升高(T >Tₛ),S 值下降。对于 x = 0.04 Sb 含量的样品,最高塞贝克系数约为 196.2 μV/K,记录于 418 K。最大的功率因数为 13.6 × 10-5 W. m-1.K-2,这是纯碲化镉在 438 K 时获得的,原因是其电导率值很高。
Antimony (Sb)-doped PbTe nanostructured alloys with improved optical and thermoelectrical characterizations for clean energy applications
The current work investigates the influence of antimony doping on the morphology, optical behavior, and thermoelectric performance of PbTe nanostructures fabricated using the hydrothermal method. Analyses employing X-ray diffraction (XRD) and Raman spectroscopy techniques asserted the existence of the cubic phase, a defining characteristic of PbTe compounds. The morphology and internal structure of the samples are examined by the scanning and high-resolution transmission electron microscopes. The photoluminescence spectra show a band gap energy around 3.0 eV which is higher than that of the bulk sample. Raman spectra show three peaks corresponding to longitudinal optical (LO) phonon mode and higher-harmonic multiphonon process of PbTe. The PL spectra exhibit a strong peak at the wavelength 401 nm which is ascribed to a recombination of excitons and/or shallowly trapped electron–hole pairs. The thermoelectric properties are studied in the temperature range of 300–500 K and confirm the domination of p-type conduction in the whole temperature range. The electrical conductivity (σ) versus temperature showed thermally activated behavior as the charge carrier mobility is activated and the average carrier kinetic energy increases with temperature. Activation energy was obtained from the plots of Ln σ as a function of 1000/T. The recorded values were found at 62, 50,73 and 34 meV for x = 0, 0.04, 0.06 and 0.08, respectively. The Seebeck coefficients (S) of the synthesized nanostructures revealed a dominance of p-type conduction due to consistently positive S values. The S-T plots exhibit an initial increase in S with temperature at lower values (T < Tₛ). However, a transition occurs at a specific temperature (Tₛ), marked by a step change in S from positive to negative values, followed by a decrease in S with further temperature rise (T > Tₛ). The highest Seebeck coefficient was observed around 196.2 μV/K and recorded at 418 K for the sample of x = 0.04 Sb content. The largest power factor was recorded at 13.6 × 10−5 W. m−1. K−2, obtained for pure PbTe at 438 K due to the high value of electrical conductivity.
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