太赫兹应用中InGaAs/InP dhbt的表面输运和直流电流增益

H. Chiang, J. Rode, P. Choudhary, M. Rodwell
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引用次数: 1

摘要

InGaAs/InP双异质结双极晶体管(dhbt)具有高击穿电压和高截止频率(fτ/fmax~0.5/1.0 THz),非常适合应用于GHz混合信号ic、>100 GHz数字逻辑、毫米波通信和成像等领域[1,2]。为了扩展HBT带宽,必须减小器件尺寸并增加InGaAs基中的掺杂浓度。结果,表面复合增加,从发射极到基极接触的横向电子传输也增加,无论是在暴露的基极表面还是在大块基极半导体内。直流电流增益(β)因此减小。实验测得太赫兹DHBTs中β为~10-25[2]。由于它限制了电路应用的有用范围,因此了解在缩放dhbt中导致β降低的机制非常重要。通过TCAD模拟,我们早前发现,基极内部的横向载流子扩散对太赫兹高温超导中观察到的高基极电流有显著贡献[3]。在这里,我们模拟了由于在暴露的半导体基底表面上的费米能级钉住而导致的发射极和基极接触之间的表面传导,并将模拟结果与实验数据进行了比较。在与fτ/fmax峰值相对应的偏置条件下,我们发现约50%的总基极电流来自表面传导。这一发现表明需要改进太赫兹高温超导的基底表面钝化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Surface transport and DC current gain in InGaAs/InP DHBTs for THz applications
InGaAs/InP double heterojunction bipolar transistors (DHBTs) are highly suitable for applications in GHz mixed-signal ICs, >100 GHz digital logic, and millimeter-wave communications and imaging because of their high breakdown voltage and high cutoff frequencies (fτ/fmax~0.5/1.0 THz)[1,2]. To extend HBT bandwidth, device dimensions must be reduced and the doping concentration in the InGaAs base must be increased. As a result, surface recombination increases, as does lateral electron transport from the emitter to the base contact, both on the exposed base surface and within the bulk base semiconductor. The DC current gain (β) thus decreases. Experimentally measured β are ~10-25 in THz DHBTs [2]. Because it limits the useful range of circuit applications, it is important to understand the mechanisms causing decreased β in scaled DHBTs. Using TCAD simulation, we had earlier found that lateral carrier diffusion within the bulk of the base contributes significantly to the observed high base currents in THz HBTs [3]. Here we model the surface conduction between the emitter and base contacts resulting from Fermi level pinning at the exposed base semiconductor surface, comparing simulations with experimental data. At bias conditions corresponding to peak fτ/fmax, we find that ~50% of the total base current arises from surface conduction. This finding suggests the need for improved base surface passivation in THz HBTs.
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