National Renewable Energy Laboratory, Golden, CO, 80401, USA.
Center for Materials Research, School of Mechanical and Materials Engineering, Washington State University, Pullman, WA, 99164-2711, USA.
Sci Rep. 2017 Jul 4;7(1):4563. doi: 10.1038/s41598-017-04719-0.
Efficient p-type doping in CdTe has remained a critical challenge for decades, limiting the performance of CdTe-based semiconductor devices. Arsenic is a promising p-type dopant; however, reproducible doping with high concentration is difficult and carrier lifetime is low. We systematically studied defect structures in As-doped CdTe using high-purity single crystal wafers to investigate the mechanisms that limit p-type doping. Two As-doped CdTe with varying acceptor density and two undoped CdTe were grown in Cd-rich and Te-rich environments. The defect structures were investigated by thermoelectric-effect spectroscopy (TEES), and first-principles calculations were used for identifying and assigning the experimentally observed defects. Measurements revealed activation of As is very low in both As-doped samples with very short lifetimes indicating strong compensation and the presence of significant carrier trapping defects. Defect studies suggest two acceptors and one donor level were introduced by As doping with activation energies at ~88 meV, ~293 meV and ~377 meV. In particular, the peak shown at ~162 K in the TEES spectra is very prominent in both As-doped samples, indicating a signature of AX-center donors. The AX-centers are believed to be responsible for most of the compensation because of their low formation energy and very prominent peak intensity in TEES spectra.
高效的 p 型掺杂在 CdTe 中仍然是几十年来的一个关键挑战,限制了基于 CdTe 的半导体器件的性能。砷是一种很有前途的 p 型掺杂剂;然而,高浓度的可重复掺杂和载流子寿命低仍然是难题。我们使用高纯度的单晶片系统地研究了砷掺杂 CdTe 的缺陷结构,以研究限制 p 型掺杂的机制。两种具有不同受主密度的砷掺杂 CdTe 和两种未掺杂的 CdTe 在富镉和富碲环境中生长。缺陷结构通过热电效应光谱(TEES)进行研究,并用第一性原理计算来确定和分配实验观察到的缺陷。测量结果表明,两种砷掺杂样品中的砷激活非常低,载流子寿命非常短,表明存在强烈的补偿和大量的载流子俘获缺陷。缺陷研究表明,砷掺杂引入了两个受主能级和一个施主能级,激活能分别约为 88meV、293meV 和 377meV。特别是,TEES 谱中在两个砷掺杂样品中都非常突出的约 162K 处的峰值表明存在 AX 中心施主的特征。由于 AX 中心的形成能低,并且在 TEES 谱中峰强度非常显著,因此它们被认为是造成大部分补偿的原因。