无基层的InP热电子晶体管在25nm宽发射极处电流密度的增加

Y. Miyamoto, I. Kashima, A. Suwa, K. Furuya
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引用次数: 0

摘要

窄发射极在降低电子器件的功耗方面是有效的。此外,它可以提供高速运行。作为这样的器件之一,我们提出了一种没有基面层的热电子晶体管[1]。在该装置中,由异质结构发射装置产生的热电子仅通过本征半导体,导致电子传播而不散射。由于固有传播区域上的正向偏置栅极调制发射器的电位,因此需要窄发射极来产生均匀的电位。正如我们之前的报告[2]所述,我们制造了一个25纳米宽的发射极,并观察了晶体管的作用。然而,观察到的电流放大电流密度约为10 A/cm2,尽管使用相同外延结构的谐振隧道二极管(RTD)显示出1 kA/cm2的峰值电流密度。为了在没有散射的情况下表现出高速性能,窄发射极中的高电流密度是必不可少的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Increase in current density at 25-nm-wide emitter for InP hot-electron transistors without base layer
A narrow emitter is effective in reducing power consumption in electron devices. Moreover, it can provide high-speed operation. As one of such devices, we proposed a hot-electron transistor without a base layer [1]. In this device, hot electrons generated by a heterostructure launcher pass through only an intrinsic semiconductor, resulting in the propagation of electrons without scattering. Because a forward-biased gate on the intrinsic propagation region modulates the potential of the launcher, a narrow emitter is required to create a uniform potential. As described in our former report [2], we fabricated a 25-nm-wide emitter and the transistor action was observed. However, the observed current density for current amplification was around 10 A/cm2, although resonant tunneling diode (RTD) using the same epitaxial structure shows a 1 kA/cm2 peak current density. To exhibit high-speed performance without scattering, high current density in a narrow emitter is essential.
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