p-n结的热电功率

Z. Dashevsky, S. Ashmontas, L. Vingelis, I. Gradauskas, A. Kasian
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引用次数: 3

摘要

在300 ~ 80 K的温度范围内,根据少数载流子的扩散长度的顺序,在掺杂层深度较大的PbTe p-n尖结上进行了热电动势测量。势垒热电动势Vb效应导致低温下输出信号急剧增加。此外,Vb的符号与体积热电动势的符号相反。势垒热电动势可以用热扩散非平衡载流子及其在pn结上的分离来解释。然而,Vb与光电动势的区别在n和p范围内是相反的符号。在这种情况下,通过仅在n范围(短激光脉冲和表层自由载流子的吸收)产生/spl δ /T来实现Vb的观测。在短脉冲(CO/sub 2/-laser /spl lambda/=10.6 /spl mu/m, /spl tau/=200 nsec)下,输出信号的增加实际上重复了激光脉冲的形式,即自由载流子的辐照吸收及其与晶格(声子系统热)的相互作用没有相互作用。与此同时,我们观察到在关闭声子系统冷却的交互作用后,信号V (/spl mu/sec)的下降非常缓慢。V的这种记忆效应不同于光电动势的响应,对于具体应用(例如测量短激光脉冲的功率)可能非常有用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The thermoelectric power on p-n junction
Measurements of thermo-EMF were performed on sharp PbTe p-n junctions with doping layer depth by order of diffusion length of minority carriers in the temperature range from 300 to 80 K. The barrier thermo-EMF Vb effect results in sharp output signal increase at low temperature. Moreover, the sign of Vb is opposite to the sign of volume thermo-EMF. The barrier thermo-EMF may be explained by thermodiffusion nonequilibrium carriers and its separation on the p-n junction. However the difference Vb from photo-EMF is an opposite sign at n- and p-ranges. In this case the observation of Vb was enabled by producing /spl Delta/T only at n-range (the absorption of short laser pulse and free carriers at surface layer). At short pulse (CO/sub 2/-laser /spl lambda/=10.6 /spl mu/m, /spl tau/=200 nsec) increase of output signal practically repeated the form of the laser pulse, i.e., irradiation absorption of free carriers and its interaction with lattice (heat of phonon system) is acting without inertion. At the same time we observed very slow decrease in signal V (/spl mu/sec and more) after switch off connecting with inertion of phonon system cooling. This memory effect of V differs from the response of photo-EMF and may be very useful for concrete applications (for example measurement of power for short laser pulse).
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