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机构地区:[1]西安交通大学电子工程系
出 处:《Journal of Semiconductors》1994年第12期850-857,共8页半导体学报(英文版)
基 金:国家教委博士点基金
摘 要:基于异质结漂移-扩散模型,考虑Fermi-Dirac统计和重掺杂能带窄变(BGN)效应,对具有非均匀掺杂基区的AlGaAs/GaAsHBT进行了数值模拟.结果表明,当基区非均匀程度较大时,非均匀掺杂引起的基区自建场远大于BGN效应产生的反向场.基区非均匀掺杂能提高电流增益,但提高的幅度随非均匀程度的增加而减慢.基区非均匀掺杂可明显改善截止频率fT,但同时也增加了集电结空间电荷区渡越时间τc,scR,使得fT在非均匀程度较大时开始下降.发射极-集电极offset电压在一定的非均匀程度下达到最佳值.本文还提出了AlGaAs/GaAsHBT基区非均匀掺杂设计的最佳条件.Abstract Numerical simulations of AlGaAs/GaAs HBTs with various base doping gradients were performed. Base doping grading is achieved by varying the doping exponentially from 1 × 1019cm-3 at the base-emitter boundary to NA2 at the basecollector boundary. The inverse built-in field due to bandgap narrowing in the base is far less than the built-in field generated by nonuniform base doping when the nonuniformity is higher. Nonuniform base doping increases the current gain, and this effect will be weakened gradually since the base-emitter SCR recombination current dominates more in the overall base current when the nonuniformity becomes higher. Base doping grading improves the cutoff frequency fT significantly, however,it also increases the base-collector SCR transit time, leading to the fall of ft. when NA2<7.5 × 1017cm-3. Tile offset voltage is improved by nonuniform base doping, and the minimum value can be obtained at NA2= 5 × 1017cm-3. An optimum base grading, NA2= 1 × 1018cm-3, is proposed.
分 类 号:TN322.8[电子电信—物理电子学]
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