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Tuning the crystallinity of thermoelectric Bi2Te3 nanowire arrays grown by pulsed electrodeposition

机译:调整通过脉冲电沉积生长的热电Bi2Te3纳米线阵列的结晶度

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Arrays of thermoelectric bismuth telluride (Bi2Te3) nanowires were grown into porous anodic alumina (PAA) membranes prepared by a two-stEP 3anodization. Bi2Te3 nanowire arrays were deposited by galvanostatic, potentiostatic and pulsed electrodeposition from aqueous solution at room temperature. Depending on the electrodeposition method and as a consequence of different growth mechanisms, Bi2Te3 nanowires exhibit different types of crystalline microstructure. Bi2Te3 nanowire arrays, especially those grown by pulsed electrodeposition, have a highly oriented crystalline structure and were grown uniformly as compared to those grown by other electrodeposition techniques used. X-ray diffraction (XRD) analyses are indicative of the existence of a preferred growth orientation. High resolution transmission electron microscopy (HRTEM) and selected area electron diffraction (SAED) confirm the formation of a preferred orientation and highly crystalline structure of the grown nanowires. The nanowires were further analyzed by scanning electron microscopy (SEM). Energy dispersive x-ray spectrometry (EDX) indicates that the composition of Bi-Te nanowires can be controlled by the electrodeposition method and the relaxation time in the pulsed electrodeposition approach. The samples fabricated by pulsed electrodeposition were electrically characterized within the temperature range 240 K <= T <= 470 K. Below T approximate to 440 K, the nanowire arrays exhibited a semiconducting behavior. Depending on the relaxation time in the pulsed electrodeposition, the semiconductor energy gaps were estimated to be 210-290 meV. At higher temperatures, as a consequence of the enhanced carrier-phonon scattering, the measured electrical resistances increased slightly. The Seebeck coefficient was measured for every Bi2Te3 sample at room temperature by a very simple method. All samples showed a positive value (12-33 mu V K-1), indicating a p-type semiconductor behavior.
机译:将热电碲化铋(Bi2Te3)纳米线的阵列生长到通过两次stEP 3阳极氧化制备的多孔阳极氧化铝(PAA)膜中。通过在室温下从水溶液中进行恒电流,恒电位和脉冲电沉积来沉积Bi2Te3纳米线阵列。取决于电沉积方法和不同生长机制的结果,Bi2Te3纳米线表现出不同类型的晶体微观结构。 Bi2Te3纳米线阵列,特别是通过脉冲电沉积生长的Bi2Te3纳米线阵列,与通过使用其他电沉积技术生长的那些相比,具有高度取向的晶体结构并且生长均匀。 X射线衍射(XRD)分析表明存在优选的生长取向。高分辨率透射电子显微镜(HRTEM)和选定区域电子衍射(SAED)证实了生长的纳米线具有较好的取向和高度结晶的结构。通过扫描电子显微镜(SEM)进一步分析纳米线。能量色散X射线能谱(EDX)表明,Bi-Te纳米线的组成可以通过电沉积方法和脉冲电沉积方法中的弛豫时间来控制。通过脉冲电沉积制备的样品在240 K <= T <= 470 K的温度范围内进行电表征。在T之下大约440 K,纳米线阵列表现出半导体性能。取决于脉冲电沉积中的弛豫时间,半导体能隙估计为210-290 meV。在更高的温度下,由于增强的载流子-声子散射,测得的电阻略有增加。用非常简单的方法在室温下测量每个Bi2Te3样品的塞贝克系数。所有样品均显示出正值(12-33μV K-1),表明其为p型半导体。

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