1.0 THz fmax InP dhbt在耐火发射极和自对准基极工艺,以减少基极接入电阻

V. Jain, J. Rode, H. Chiang, A. Baraskar, E. Lobisser, B. Thibeault, M. Rodwell, M. Urteaga, D. Loubychev, A. Snyder, Y. Wu, J. Fastenau, W.K. Liu
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引用次数: 23

摘要

我们报道了220 nm InP双异质结双极晶体管(dhbt),其fτ = 480 GHz, fmax = 1.0 THz。发射极和基极工艺的改进使得即使在220 nm宽的发射极-基极结和1.1 μ m宽的基极-集电极台面上也可以实现1.0 THz的fmax。垂直发射极金属蚀刻轮廓,湿蚀刻薄的InP发射极半导体具有小于10 nm的凹边和自对准基极接触沉积,将发射极半导体基极金属间隙(Wgap)减少到~ 10 nm,从而显着降低总基极存取电阻(Rbb)中的间隙电阻项(Rgap),从而实现高fmax器件。通过在基柱下方的基台凹边减小总集电极基电容(Ccb),进一步提高了fmax。这些器件采用Mo/W/TiW耐火发射极金属触点,允许在高发射极电流密度(Je)下对晶体管进行偏置,而不会出现电应力下的电迁移或触点扩散问题[1]。
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1.0 THz fmax InP DHBTs in a refractory emitter and self-aligned base process for reduced base access resistance
We report 220 nm InP double heterojunction bipolar transistors (DHBTs) demonstrating fτ = 480 GHz and fmax = 1.0 THz. Improvements in the emitter and base processes have made it possible to achieve a 1.0 THz fmax even at 220 nm wide emitter-base junction with a 1.1 µm wide base-collector mesa. A vertical emitter metal etch profile, wet-etched thin InP emitter semiconductor with less than 10 nm undercut and self-aligned base contact deposition reduces the emitter semiconductor-base metal gap (Wgap) to ∼ 10 nm, thereby significantly reducing the gap resistance term (Rgap) in the total base access resistance (Rbb), enabling a high fmax device. Reduction in the total collector base capacitance (Ccb) through undercut in the base mesa below base post further improved fmax. These devices employ a Mo/W/TiW refractory emitter metal contact which allows biasing the transistors at high emitter current densities (Je) without problems of electromigration or contact diffusion under electrical stress [1].
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