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1.
This paper describes the fabrication and characteristics of small-scaled InGaP/GaAs HBTs with high-speed as well as low-current operation. To reduce both the emitter size SE and the base-collector capacitance CBC simultaneously, the HBTs are fabricated by using WSi/Ti as the base electrode and by burying SiO2 in the extrinsic base-collector region under the base electrode. WSi/Ti simplifies and facilitates processing to fabricate a small base electrode, and makes it possible to reduce the width of the base contact to less than 0.4 μm without the large increase in the base resistance. The DC current gain of 20 is obtained for an HBT with S E of 0.3×1.6 μm2 due to the suppression of emitter size effect by using InGaP as the emitter material. An HBT with SE of 0.6×4.6 μm2 exhibited fT of 138 GHz and fmax of 275 GHz at IC of 4 mA; and an HBT with SE of 0.3×1.6 μm2 exhibited fT of 96 GHz and fmax of 197 GHz at IC of 1 mA. These results indicate the great potential of these HBTs for high-speed and low-power circuit applications  相似文献   

2.
This paper describes a novel fully planar AlGaAs/GaAs heterojunction bipolar transistor (HBT) technology using selective chemical beam epitaxy (CBE). Planarization is achieved by a selective regrowth of the base and collector contact layers. This process allows the simultaneous metallization of the emitter, base and collector on top of the device. For the devices with an emitter-base junction area of 2×6 μm2 and a base-collector junction area of 14×6 μm2, a current gain cut off frequency of 50 GHz and a maximum oscillation frequency of 30 GHz are achieved. The common emitter current gain hFE is 25 for a collector current density Jc of 2×104 A/cm2  相似文献   

3.
A self-aligned process is developed to obtain submicrometer high-performance AlGaAs/GaAs heterojunction bipolar transistors (HBTs) which can maintain a high current gain for emitter sizes on the order of 1 μm2. The major features of the process are incorporation of an AlGaAs surface passivation structure around the entire emitter-base junction periphery to reduce surface recombination and reliable removal of base metal (Ti/W) deposits from the sidewall by electron cyclotron resonance (ECR) plasma deposition of oxide and ECR plasma etching by NF3. A DC current gain of more than 30 can be obtained for HBTs with an emitter-base junction area of 0.5×2 μm2 at submilliampere collector currents. The maximum fT and fmax obtained from a 0.5×2 μm2 emitter HBT are 46 and 42 GHz, respectively at IC=1.5 and more than 20 GHz even at IC=0.1 mA  相似文献   

4.
GaInP-GaAs heterojunction bipolar phototransistors grown by metal organic vapor phase epitaxy (MOVPE) and operated with frontside optical injection through the emitter are reported with high optical gain (<88) and record high frequency performance (28 GHz). Heteropassivation of the extrinsic base surface is employed using a depleted GaInP emitter layer between the nonself-aligned base contact and the emitter mesa. The phototransistor's performance is shown to improve with increasing dc base bias in agreement with predictions of a recently reported Gummel-Poon model. Experimental results are reported for devices with optical active areas of 10×10 μm2, 20×20 μm2, and 30×30 μm2, with peak measured cutoff frequencies of 28.5, 23.1, and 18.5 GHz, respectively, obtained at collector current densities between 2×10 3 and 6×103 A/cm2  相似文献   

5.
The total emitter to collector delay for a Pnp AlGaAs/GaAs HBT has been reduced to 4.8 ps by employing a thin base (325 Å) and collector (2300 Å). Simultaneously, a low base sheet resistance of 170 ohms/square was achieved with tellurium doping. A higher collector doping than is typically used permitted operation at collector current densities in excess of 5×104 A/cm2. A single emitter (2×4 μm2) and a single base contact device topology has an ft and fmax of 33 and 66 GHz, respectively  相似文献   

6.
We examine the geometrical scaling issues in SiGe HBT technology. Width Scaling, length scaling, and stripe-number scaling are quantified from a radio frequency (RF) design perspective at 2 GHz. We conclude that a SiGe HBT with emitter area AE=0.5×20×6 μm2 is optimum for low noise applications at Jc=0.1 mA/μm2 and f=2 GHz using the design methodology, which guarantees optimal noise and input impedance matching with the simplest matching network. Finally, the optimal device sizes at f=4 and 6 GHz for low noise applications are also obtained using the same method  相似文献   

7.
Self-aligned AlGaAs/GAs heterojunction bipolar transistors with peak specific transconductances as high as 25 mS/μm2 of emitter area are discussed. These are the highest specific transconductances ever reported for a bipolar transistor. These devices, which contain no indium in the emitter, display specific parasitic emitter resistances of less than 1×10-7 Ω-cm2. This low parasitic resistance is attributed to an improved n-type contact technology, in which a molybdenum diffusion barrier and a plasma-enhanced chemical vapor deposition SiO2 overlayer are used to achieve low specific contact resistivities  相似文献   

8.
A high-performance 0.5-μm BiCMOS technology has been developed. Three layers of polysilicon are used to achieve a compact four-transistor SRAM bit cell size of less than 20 μm2 by creating self-aligned bit-sense and Vss contacts. A WSix polycide emitter n-p-n transistor with an emitter area of 0.8×2.4 μm2 provides a peak cutoff frequency (fT) of 14 GHz with a collector-emitter breakdown voltage (BVCFO) of 6.5 V. A selectively ion-implanted collector (SIC) is used to compensate the base channeling tail in order to increase fT and knee current without significantly affecting collector-substrate capacitance. ECL gate delays as fast as 105 ps can be obtained with this process  相似文献   

9.
A high performance BiCMOS technology, BEST2 (Bipolar Enhanced super Self-aligned Technology) designed for supporting low-power multiGHz mixed-signal applications is presented. Process modules to produce low parasitic device structures are described. The developed BiCMOS process implemented with 1 μm design rules (0.5 μm as one nesting tolerance) has achieved fl and fmax for npn bipolar (Ae=1×2 μm2) of 23 GHz and 24 GHz at Vce=3 V, respectively, with BVceo⩾5.5 volts, and βVA product of 2400. Typical measured ECL gate delay is 48 ps/37 ps per stage (Ae=1×2 μm2 ; 500 mV swing) at 0.6 mA/2.1 mA switching currents, and CMOS gate delay (gate oxide=125 Å, Leff=0.6 μm; Vth,nch =0.45 V; Vth,pch=-0.45 V) 70 ps/stage. A BiCMOS phase-locked-loop (emitter width=1 μm; gate Leff=0.7 μm) has achieved 6 GHz operation at 2 V power supply with total power consumption of 60 mW  相似文献   

10.
A theoretical investigation of Si/Si1-xGex heterojunction bipolar transistors (HBTs) undertaken in an attempt to determine their speed potential is discussed. The analysis is based on a compact transistor model, and devices with self-aligned geometry, including both extrinsic and intrinsic parameters, are considered. For an emitter area of 1×5 μm2, an ft of over 75 GHz and fmax of over 35 GHz were computed at a collector current density of 1×10 5 A/cm2 and VCB of 5 V  相似文献   

11.
This letter describes the material characterization and device test of InAlAs/InGaAs high electron mobility transistors (HEMTs) grown on GaAs substrates with indium compositions and performance comparable to InP-based devices. This technology demonstrates the potential for lowered production cost of very high performance devices. The transistors were fabricated from material with room temperature channel electron mobilities and carrier concentrations of μ=10000 cm2 /Vs, n=3.2×1012 cm-2 (In=53%) and μ=11800 cm2/Vs, n=2.8×1012 cm-2 (In=60%). A series of In=53%, 0.1×100 μm2 and 0.1×50 μm2 devices demonstrated extrinsic transconductance values greater than 1 S/mm with the best device reaching 1.074 S/mm. High-frequency testing of 0.1×50 μm2 discrete HEMT's up to 40 GHz and fitting of a small signal equivalent circuit yielded an intrinsic transconductance (gm,i) of 1.67 S/mm, with unity current gain frequency (fT) of 150 GHz and a maximum frequency of oscillation (fmax) of 330 GHz. Transistors with In=60% exhibited an extrinsic gm of 1.7 S/mm, which is the highest reported value for a GaAs based device  相似文献   

12.
This paper reports on SiGe NPN HBTs with unity gain cutoff frequency (fT) of 207 GHz and an fMAX extrapolated from Mason's unilateral gain of 285 GHz. fMAX extrapolated from maximum available gain is 194 GHz. Transistors sized 0.12×2.5 μm2 have these characteristics at a linear current of 1.0 mA/μm (8.3 mA/μm2). Smaller transistors (0.12×0.5 μm2) have an fT of 180 GHz at 800 μA current. The devices have a pinched base sheet resistance of 2.5 kΩ/sq. and an open-base breakdown voltage BVCEO of 1.7 V. The improved performance is a result of a new self-aligned device structure that minimizes parasitic resistance and capacitance without affecting fT at small lateral dimensions  相似文献   

13.
High-performance InP/In0.53Ga0.47As metamorphic heterojunction bipolar transistors (MHBTs) on GaAs substrate have been fabricated using InxGa1-xP strain relief buffer layer grown by solid-source molecular beam epitaxy (SSMBE). The MHBTs exhibited a dc current gain over 100, a unity current gain cutoff frequency (fT) of 48 GHz and a maximum oscillation frequency (fMAX) of 42 GHz with low junction leakage current and high breakdown voltages. It has also been shown that the MHBTs have achieved a minimum noise figure of 2 dB at 2 GHz (devices with 5×5 μm 2 emitter) and a maximum output power of 18 dBm at 2.5 GHz (devices with 5×20 μm2 emitter), which are comparable to the values reported on the lattice-matched HBTs (LHBTs). The dc and microwave characteristics show the great potential of the InP/InGaAs MHBTs on GaAs substrate for high-frequency and high-speed applications  相似文献   

14.
The microwave and power performance of fabricated InP-based single and double heterojunction bipolar transistors (HBTs) is presented. The single heterojunction bipolar transistors (SHBTs), which had a 5000 Å InGaAs collector, had BVCEO of 7.2 V and JCmax of 2×105 A/cm2. The resulting HBTs with 2×10 μm2 emitters produced up to 1.1 mW/μm2 at 8 GHz with efficiencies over 30%. Double heterojunction bipolar transistors (DHBTs) with a 3000-Å InP collector had a BVCEO of 9 V and Jc max of 1.1×105 A/cm2, resulting in power densities up to 1.9 mW/μm2 at 8 GHz and a peak efficiency of 46%. Similar DHBTs with a 6000 Å InP collector had a higher BVCEO of 18 V, but the J c max decreased to 0.4×105 A/cm2 due to current blocking at the base-collector junction. Although the 6000 Å InP collector provided higher fmax and gain than the 3000 Å collector, the lower Jc max reduced its maximum power density below that of the SHBT wafer. The impact on power performance of various device characteristics, such as knee voltage, breakdown voltage, and maximum current density, are analyzed and discussed  相似文献   

15.
In-situ boron-doped polysilicon has been used to form the emitter in p-n-p transistors. Various polysilicon deposition conditions, interface preparation treatments prior to deposition, and post-deposition anneals were investigated. Unannealed devices lacking a deliberately grown interfacial oxide gave effective emitter Gummel numbers GE of 7-9×10-12s cm-4 combined with emitter resistances RE of approximately 8 μΩcm2. Introduction of a chemically grown interfacial oxide increased GE to 2×10 14s cm-4, but also raised RE by a factor of three. Annealing at 900°C following polysilicon deposition raised GE values for transistors lacking deliberate interfacial oxide to approximately 6×1013s cm-4, but had little effect of GE for devices with interfacial oxide. Both types of annealed devices gave RE values in the range 1-2 μΩcm2  相似文献   

16.
High-gain GaAs/AlGaAs n-p-n heterojunction bipolar transistors (HBT's) on Si substrates grown by molecular beam epitaxy (MBE) have been fabricated and tested. In this structure, an n+-InAs emitter cap layer was grown in order to achieve a nonalloyed ohmic contact. Typical devices with an emitter dimension of 50×50 μm2 exhibited a current gain as high as 45 at a collector current density of 2×103 A/cm2 with an ideality factor of 1.4. This is the highest current gain reported for HBT's grown on Si substrates. Breakdown voltages as high as 10 and 15 V were observed for the emitter-base and collector-base junctions respectively. The investigation on devices with varying emitter dimensions demonstrates that much higher current gains can be expected  相似文献   

17.
The high speed scaling of an Al0.48In0.52As/In0.53Ga0.47 As submicrometer heterostructure bipolar transistor (HBT) is presented. Transistors with emitter dimensions of 0.5×11 and 3.5×3.5 μm2 exhibit unity current-gain cutoff frequencies of 63 and 70 GHz, respectively. Emitter current density greater than 3.3×105 A/cm2 is demonstrated in a submicrometer AlInAs/InGaAs HBT. The analysis shows that the device speed is limited by the parasitic collector charging time  相似文献   

18.
We report on the microwave performance of InP/In0.53Ga 0.47As heterojunction bipolar transistors (HBT's) utilizing a carbon-doped base grown by chemical beam epitaxy (CBE). The fT and fmax of the HBT having two 1.5×10 μm2 emitter fingers were 175 GHz and 70 GHz, respectively, at IC=40 mA and VCE=1.5 V. To our knowledge, the f T of this device is the highest of any type of bipolar transistors yet reported. These results indicate the great potential of carbon-doped base InP/InGaAs HBT's for high-speed applications  相似文献   

19.
We have developed the advanced performance, small-scale InGaP/GaAs heterojunction bipolar transistors (HBTs) by using WSi/Ti base electrode and buried SiO2 in the extrinsic collector. The base-collector capacitance CBC was further reduced to improve high-frequency performance. Improving the uniformity of the buried SiO 2, reducing the area of the base electrode, and optimizing the width of the base-contact enabled us to reduce the parasitic capacitance in the buried SiO2 region by 50% compared to our previous devices. The cutoff frequency fT of 156 GHz and the maximum oscillation frequency fmax of 255 GHz were obtained at a collector current IC of 3.5 mA for the HBT with an emitter size SE of 0.5×4.5 μm2, and fT of 114 GHz and fmax of 230 GHz were obtained at IC of 0.9 mA for the HBT with SE of 0.25×1.5 μm2. We have also fabricated digital and analog circuits using these HBTs. A 1/8 static frequency divider operated at a maximum toggle frequency of 39.5 GHz with a power consumption per flip-flop of 190 mW. A transimpedance amplifier provides a gain of 46.5 dB·Ω with a bandwidth of 41.6 GHz at a power consumption of 150 mW. These results indicate the great potential of our HBTs for high-speed, low-power circuit applications  相似文献   

20.
The authors demonstrate excellent passivation of the extrinsic base surfaces in GaInP/GaAs heterojunction bipolar transistors (HBTs) having small emitter areas. Passivated devices with an area as small as 4×20 μm2 exhibit the highest reported current gain value of 2690 for GaInP/GaAs HBTs, while unpassivated 4×20-μm 2 devices exhibit a current gain of only 500. Measured current gains as a function of collector current density are almost identical for devices with varying emitter widths of 4, 6, 8, 12, 16, and 100 μm. The current gains are also nearly identical for devices with varying passivation ledge widths of 1, 2, 3, and 6 μm. These results are contrasted with those of a previously published study reporting surface passivation for a GaInP/GaAs HBT with a large emitter area  相似文献   

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