内置极化效应对InGaN/GaN异质结构热电效率的影响

B. Sahoo
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引用次数: 1

摘要

GaN/InxGa1−xN /GaN超晶格(SLs)的热电效率要求Seebeck系数(S)和电导率(σ)达到最大值;但导热系数(k)最小,k越小,TE的优值(ZT)越高。GaN/InxGa1−xN /GaN SLs的内置极化(BIP)提高了SLs的S和σ,但BIP对k的作用尚未研究。本文从理论上计算了BIP对GaN/InxGa1−xN /GaN SLs k的影响。SL的BIP提高了InxGa1−xN在室温下的德拜温度、声子平均自由程和导热系数。热导率(kp:含极化机制和k:不含极化机制)随温度的变化预示着两种热导率出现交叉的转变温度(Tp)的存在。在Tp以下,kp小于k;而在Tp以上,kp主要由热膨胀引起的BIP机制贡献。这表明了SL的多孔性。已经证明Tp依赖于x,应变和由于界面而产生的边界电阻。因此,通过调整材料的成分、应变和界面电阻,可以根据需要修改SL的导热系数。该研究将有助于优化模块的几何形状(no. 1)。界面,井和屏障的厚度,热元件的长度和无。(SLs中的周期)以获得最大发电量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Built in polarization effect on thermoelectric efficiency of InGaN/GaN heterostructure
The superior thermoelectric (TE) efficiency of GaN/InxGa1−xN /GaN superlattice (SLs) requires maximum values of Seebeck coefficient (S) and electrical conductivity (σ); but minimum value of thermal conductivity (k). A smaller k would lead to even further increase of TE figure of merit (ZT). The built in polarization (BIP) of GaN/InxGa1−xN /GaN SLs enhances S and σ of the SLs, however role of BIP on k has not been explored. In this work the effect of BIP on k of GaN/InxGa1−xN /GaN SLs has been computed theoretically. The BIP of SL enhances Debye temperature, phonon mean free path and thermal conductivity of InxGa1−xN at room temperature. The variation of thermal conductivities (kp: including polarization mechanism and k: without polarization mechanism) with temperature predicts the existence of a transition temperature (Tp) where both thermal conductivities show crossover. Below Tp, kp is lower than k; while above Tp, kp is significantly contributed from BIP mechanism due to thermal expansion. This signifies poyroelectric behavior of SL. It has been shown that Tp depends on x, strain and boundary resistance due to interfaces. Thus, tailoring the In composition, strain and interface resistance, thermal conductivity of the SL can be modified as per requirement. This study will be useful for optimization of module geometry (no. of interfaces, thickness of well and barriers, length of thermo-elements and no. of periods in SLs) for maximum power generation.
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