首页> 外文期刊>Journal of Crystal Growth >Impact of strained GaAs spacer between InP emitter and GaAs_(1-y)Sb_y base on structural properties and electrical characteristics of MOCVD-grown InP/GaAs_(1-y)Sb_y/InP DHBTs
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Impact of strained GaAs spacer between InP emitter and GaAs_(1-y)Sb_y base on structural properties and electrical characteristics of MOCVD-grown InP/GaAs_(1-y)Sb_y/InP DHBTs

机译:InP发射极和GaAs_(1-y)Sb_y之间应变的GaAs隔离层对MOCVD生长的InP / GaAs_(1-y)Sb_y / InP DHBTs的结构性能和电学特性的影响

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摘要

Novel InP/GaAs_(1-y)Sb_y/InP double-heterojunction bipolar transistors (HBTs) with a GaAs spacer between the InP emitter and GaAs_(1-y)Sb_y base layer were grown by the metalorganic chemical vapor deposition method in order to simplify the switching sequence for forming a high-quality InP-emitter/GaAs_(1-y)Sb_y-base interface. After removal of the InP emitter, the top surface of the GaAs spacer exhibits smooth step-flow-like morphology with root-mean-square roughness of 0.17-0.36 nm, whereas the morphology of the GaAs_(1-y)Sb_y, base of the sample without the GaAs spacer is bumpy. Secondary ion mass spectroscopy reveals that the spacer suppresses the incorporation of excess Sb into the InP emitter around the emitter-base junction. The dependence of the current gain on the thickness of the GaAs spacer is investigated and, when the GaAs spacer is 2 nm, the highest current gain is obtained. Therefore, we employ the spacer to scaled-down HBTs with a 0.25-μm-wide emitter. The scaled-down HBTs show high current gain of over 90 at collector current density J_c of 10 mA/μm~2 even though the space between emitter and base electrodes is just 0.15 μm. We obtain peak current-gain cut-off frequency of 388 GHz and peak maximum oscillation frequency of 290 GHz at J_c = 10 mA/μm~2. This result suggests that the presence of the GaAs spacer does not impose any penalty on the characteristics at high J_c. The insertion of the GaAs spacer is a good way to obtain a high-quality E-B interface with a simple precursor-supply sequence and thereby HBTs with both high-current gain and reasonably high RF performance.
机译:通过金属有机化学气相沉积法生长了在InP发射极和GaAs_(1-y)Sb_y基极层之间具有GaAs间隔层的新型InP / GaAs_(1-y)Sb_y / InP双异质结双极晶体管(HBT),以便简化了形成高质量InP发射极/ GaAs_(1-y)Sb_y基接口的开关顺序。去除InP发射极后,GaAs间隔层的顶面呈现出平滑的阶梯状流动形态,均方根粗糙度为0.17-0.36 nm,而GaAs_(1-y)Sb_y的形态为没有GaAs隔离层的样品是颠簸的。二次离子质谱表明,隔离物抑制了过量的Sb结合到发射极-基极结周围的InP发射极中。研究了电流增益对GaAs隔离层厚度的依赖性,当GaAs隔离层为2 nm时,可获得最高的电流增益。因此,我们采用隔离层来缩小0.25μm宽发射极的HBT。按比例缩小的HBT在集电极电流密度J_c为10 mA /μm〜2时显示出超过90的高电流增益,即使发射极和基极之间的空间仅为0.15μm。在J_c = 10 mA /μm〜2时,我们获得了388 GHz的峰值电流增益截止频率和290 GHz的峰值最大振荡频率。该结果表明,GaAs间隔物的存在不会对高J_c下的特性造成任何不利影响。 GaAs隔离层的插入是获得具有简单前驱物供应顺序的高质量E-B界面的好方法,从而获得具有高电流增益和相当高的RF性能的HBT。

著录项

  • 来源
    《Journal of Crystal Growth》 |2014年第1期|31-37|共7页
  • 作者单位

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

    NTT Photonics Laboratories, NTT Corporation 3-1 Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243 0198, Japan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    A3. Metalorganic chemical vapor deposition; B1. Antimonides; B3. Bipolar transistors;

    机译:A3。金属有机化学气相沉积;B1。锑化物;B3。双极晶体管;
  • 入库时间 2022-08-17 13:14:11

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