GaAs双极结构中的相互扩散

W. Li, R. M. Cohen, D. Simons, P. Chi
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引用次数: 0

摘要

采用有机金属气相外延(OMVPE)法制备了标称厚度为0.5 /spl mu/m的GaAs发射极层、基极层和集电极层。每一层都含有互扩散标记物铟的浓度峰。退火在开管系统中进行1小时,温度为900/spl度/C,砷压力可控。所使用的掺杂剂碲和碳驻留在V族亚晶格上,预计它们不会诱发所谓的踢出扩散机制。测量的相互扩散结果与退火过程中接近平衡值的缺陷浓度一致。对于npn结构,可以测量到一个小的发射极推进效应。我们发现,在载流子密度n=1/spl乘以/10/sup 19/ cm/sup -3/到p=1/spl乘以/10/sup 19/ cm/sup -3/范围内,带-1电荷的Ga空位为n型和p型GaAs的相互扩散提供了一致的解释。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Interdiffusion in GaAs bipolar structures
Emitter, base, and collector layers of GaAs with a nominal thickness of 0.5 /spl mu/m each were grown by organometallic vapor phase epitaxy (OMVPE). Each layer contained concentration spikes of the interdiffusion marker, indium. Annealing was performed in an open tube system for 1 h at T=900/spl deg/C using a controlled arsenic pressure. The dopants used, tellurium and carbon, reside on the group V sublattice and they are not expected to induce the so-called kick-out diffusion mechanism. The measured interdiffusion results are consistent with native defect concentrations' which approach their equilibrium values during the annealing process. A small emitter push effect can be measured for npn structures. We find that a Ga vacancy, with a charge of -1, provides a consistent explanation for interdiffusion in both n-type and p-type GaAs over the range of carrier density n=1/spl times/10/sup 19/ cm/sup -3/ to p=1/spl times/10/sup 19/ cm/sup -3/.
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