TY - JOUR
T1 - InGaAs-GaAs pseudomorphic heterostructure transistors prepared by MOVPE
AU - Liu, Wen Chau
AU - Laih, Lih Wen
AU - Tsai, Jung Hui
AU - Lin, Kun Wei
AU - Cheng, Chin Chuan
PY - 1997/1
Y1 - 1997/1
N2 - In this paper, we will demonstrate two new InGaAs-GaAs pseudomorphic heterostructure transistors prepared by MOVPE technology, i.e. InGaAs-GaAs graded-concentration doping-channel MIS-like field effect transistors (FET) and heterostructure-emitter and heterostructure-base (InGaAs-GaAs) transistors (HEHBT). For the doping-channel MIS-like FET, the graded In0.15Ga0.85As doping-channel structure is employed as the active channel. For a 0.8 × 100 μm2 gate device, a breakdown voltage of 15 V, a maximum transconductance of 200 mS/mm, and a maximum drain saturation current of 735 mA/mm are obtained. For the HEHBT, the confinement effect for holes is enhanced owing to the presence of GaAs/InGaAs/GaAs quantum wells. Thus, the emitter injection efficiency is increased and a high current gain can be obtained. Also, due to the lower surface recombination velocity of InGaAs base layers, the potential spike of the emitter-base (E-B) junction can be reduced significantly. This can provide a lower collector-emitter offset voltage. For an emitter area of 4.9 × 10-5 cm2, the common emitter current gain of 120 and the collector-emitter offset voltage of 100 mV are obtained.
AB - In this paper, we will demonstrate two new InGaAs-GaAs pseudomorphic heterostructure transistors prepared by MOVPE technology, i.e. InGaAs-GaAs graded-concentration doping-channel MIS-like field effect transistors (FET) and heterostructure-emitter and heterostructure-base (InGaAs-GaAs) transistors (HEHBT). For the doping-channel MIS-like FET, the graded In0.15Ga0.85As doping-channel structure is employed as the active channel. For a 0.8 × 100 μm2 gate device, a breakdown voltage of 15 V, a maximum transconductance of 200 mS/mm, and a maximum drain saturation current of 735 mA/mm are obtained. For the HEHBT, the confinement effect for holes is enhanced owing to the presence of GaAs/InGaAs/GaAs quantum wells. Thus, the emitter injection efficiency is increased and a high current gain can be obtained. Also, due to the lower surface recombination velocity of InGaAs base layers, the potential spike of the emitter-base (E-B) junction can be reduced significantly. This can provide a lower collector-emitter offset voltage. For an emitter area of 4.9 × 10-5 cm2, the common emitter current gain of 120 and the collector-emitter offset voltage of 100 mV are obtained.
UR - http://www.scopus.com/inward/record.url?scp=0030687701&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0030687701&partnerID=8YFLogxK
U2 - 10.1016/S0022-0248(96)00502-7
DO - 10.1016/S0022-0248(96)00502-7
M3 - Article
AN - SCOPUS:0030687701
SN - 0022-0248
VL - 170
SP - 438
EP - 441
JO - Journal of Crystal Growth
JF - Journal of Crystal Growth
IS - 1-4
ER -