Title: 185 GHz Monolithic Amplifier in InGaAs/InAlAs Transferred-Substrate HBT Technology
1185 GHz Monolithic Amplifier in InGaAs/InAlAs
Transferred-Substrate HBT Technology
M. Urteaga, D. Scott, T. Mathew, S. Krishnan, Y.
Wei, M. Rodwell. Department of Electrical and
Computer Engineering, University of California,
Santa Barbara
urteaga_at_ece.ucsb.edu 1-805-893-8044
IMS2001 May 2001, Phoenix, AZ
2Outline
IMS2001
UCSB
- Introduction
- Transferred-Substrate HBT Technology
- Circuit Design
- Results
- Conclusion
3Transferred-Substrate HBTs
IMS2001
- Substrate transfer allows simultaneous scaling
of emitter and collector widths - Maximum frequency of oscillation
-
- Sub-micron scaling of emitter and collector
widths has resulted in record values for
extrapolated fmax (gt1 THz) - Promising technology for ultra-high frequency
tuned circuit applications
30
Mason's
3000 Å collector 400 Å base with 52 meV
grading AlInAs / GaInAs / GaInAs HBT
gain, U
25
20
MSG
Gains, dB
H
f
1.1 THz ??
21
max
f
204 GHz
Emitter, 0.4 x 6 mm2
t
Collector, 0.7 x 6 mm2
I
6 mA, V
1.2 V
c
ce
10
100
1000
Frequency, GHz
4Ultra-high Frequency Amplifiers
IMS2001
- Applications for electronics in 140-220 GHz
frequency band - Wideband communication systems
- Atmospheric sensing
- Automotive radar
- Amplifiers in this frequency band realized in
InP-based HEMT technologies - 3-stage amplifier with 30 dB gain at 140 GHz.
- Pobanz et. al., IEEE JSSC, Vol. 34, No. 9,
Sept. 1999. - 3-stage amplifier with 12-15 dB gain from
160-190 GHz - Lai et. al., 2000 IEDM, San Francisco, CA.
- 6-stage amplifier with 20 ? 6 dB from 150-215
GHz. - Weinreb et. al., IEEE MGWL, Vol. 9, No. 7,
Sept. 1999. - This Work
- Single-stage tuned amplifier with 3.0 dB gain at
185 GHz - First HBT amplifier in this frequency range
- Gain-per-stage is comparable to HEMT technology
-
5InGaAs/InAlAs HBT Material System
IMS2001
Layer Structure
Band Diagram
2kT base bandgap grading
Bias conditions for the band diagram Vbe 0.7
V Vce 0.9 V
6 Device Fabrication I
IMS2001
7 Transferred-Substrate Process Flow
IMS2001
- emitter metal
- emitter etch
- self-aligned base
- mesa isolation
-
- polyimide planarization
- interconnect metal
- silicon nitride insulation
- Benzocyclobutene, etch vias
- electroplate gold
- bond to carrier wafer with solder
- remove InP substrate
- collector metal
- collector recess etch
8 Device Fabrication II
IMS2001
9Ultra-high fmax Devices
IMS2001
- Electron beam lithography used to define
submicron emitters and collectors - Minimum feature sizes
- 0.2 ?m emitter stripe widths
- 0.3 ?m collector stripe widths
- Improved collector-to-emitter alignment using
local alignment marks - Future Device Improvements
- Carbon base doping
- na gt1.0 x 1020 cm-3
- significant reduction in Rbb
- DHBTs with InP Collectors
- Greater than 6 V BVCEO
0.3 ?m Emitter before polyimide planarization
0.4 ?m Collector Stripe
10Device Measurements
IMS2001
DC Measurements
Measured RF Gains
- Device dimensions
- Emitter area 0.4 x 6 ?m2
- Collector area 0.7 x 6.4 ?m2
- ? 20
- BVCEO 1.5 V
- Bias Conditions
- VCE 1.2 V, IC 4.8 mA
- f? 160 GHz
- Measurements of unilateral power gain in
140-220 GHz frequency band appear to show
unphysical behavior
11Amplifier Design
IMS2001
Simulation Results
- Simple common-emitter design conjugately matched
at 200 GHz using shunt-stub tuning - Shunt R-C network at output provides low
frequency stabilization - Simulations predicted 6.2 dB gain
- Designed using hybrid-pi model derived from
DC-50 GHz measurements of previous generation
devices - Electromagnetic simulator (Agilents Momentum)
was used to characterize critical passive
elements
S21
S11, S22
Circuit Schematic
12IMS2001
Design Considerations in Sub-mmwave Bands
- Transferred-substrate technology provides low
inductance microstrip wiring environment - Ideal for Mixed Signal ICs
- Advantages for MMIC design
- Low via inductance
- Reduced fringing fields
- Disadvantages for MMIC design
- Increased conductor losses
- Resistive losses are inversely proportional to
the substrate thickness for a given Zo - Amplifier simulations with lossless matching
network showed 2 dB more gain - Possible Solutions
- Use airbridge transmission lines
- Find optimum substrate thickness
13140-220 GHz VNA Measurements
IMS2001
- HP8510C VNA used with Oleson Microwave Lab
mmwave Extenders - Extenders connected to GGB Industries coplanar
wafer probes via short length of WR-5 waveguide - Internal bias Tees in probes for biasing active
devices - Full-two port T/R measurement capability
- Line-Reflect-Line calibration performed using
on-wafer transmission line standards
UCSB 140-220 GHz VNA Measurement Set-up
14Amplifier Measurements
IMS2001
- Measured 3.0 dB peak gain at 185 GHz
- Device dimensions
- Emitter area 0.4 x 6 ?m2
- Collector area 0.7 x 6.4 ?m2
- Device bias conditions
- Ic 3.0 mA, VCE 1.2 V
Measured Gain
Measured Return Loss
Cell Dimensions 690?m x 350 ?m
15Simulation vs. Measurement
IMS2001
Simulation versus Measured Results
- Amplifier designed for 200 GHz
- Peak gain measured at 185 GHz
- Possible sources for discrepancy
- Matching network design
- Device model
16Matching Network Design
IMS2001
Matching Network Breakout Simulation Vs.
Measurement
- Breakout of matching network without active
device was measured on-wafer - Measurement compared to circuit simulation of
passive components - Simulations show good agreement with measurement
- Verifies design approach of combining E-M
simulation of critical passive elements with
standard microstrip models
S21
S11
S22
Red- Simulation Blue- Measurement
17Device Modeling I Hybrid-Pi Model
IMS2001
HBT Hybrid-Pi Model Derived from DC-50 GHz
Measurements
- Design used a hybrid-pi device model based on
DC-50 GHz measurements - Measurements of individual devices in 140-220
GHz band show poor agreement with model - Discrepancies may be due to weakness in device
model and/or measurement inaccuracies - Device dimensions
- Emitter area 0.4 x 6 ?m2
- Collector area 0.7 x 6.4 ?m2
- Bias Conditions
- VCE 1.2 V, IC 4.8 mA
18IMS2001
Device Modeling II Model vs. Measurement
S21
- Measurements and simulations of device
S-parameters from 6-45 GHz and 140-220 GHz - Large discrepancies in S11 and S22
- Anomalous S12 believed to be due to excessive
probe-to-probe coupling - Red- Simulation
- Blue- Measurement
S11, S22
S12
19Simulation vs. Measurement
IMS2001
UCSB
Simulation versus Measured Results Simulation
Using Measured Device S-parameters
- Simulated amplifier using measured device
S-parameters in the 140-220 GHz band - Simulations show better agreement with measured
amplifier results - Results point to weakness in hybrid-pi model
used in the design - Improved device models are necessary for better
physical understanding but measured S-parameter
can be used in future amplifier designs
20Conclusions
IMS2001
UCSB
- Demonstrated first HBT amplifier in the 140-220
GHz frequency band - Simple design provides direction for future high
frequency MMIC work in transferred-substrate
process - Observed anomalies in extending hybrid-pi model
to higher frequencies - Future Work
- Multi-stage amplifiers and oscillators
- Improved device performance for higher frequency
operation - Acknowledgements
- This work was supported by the ONR under grant
N0014-99-1-0041 - And the AFOSR under grant F49620-99-1-0079