Single-stage G-band HBT Amplifier with 6.3 dB Gain at 175 GHz - PowerPoint PPT Presentation

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Single-stage G-band HBT Amplifier with 6.3 dB Gain at 175 GHz

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Title: No Slide Title Author: Miguel Urteaga Keywords: HBT presentation Last modified by: urteaga Created Date: 3/6/2001 3:46:39 PM Document presentation format – PowerPoint PPT presentation

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Title: Single-stage G-band HBT Amplifier with 6.3 dB Gain at 175 GHz


1
Single-stage G-band HBT Amplifier with 6.3 dB
Gain at 175 GHz
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
GaAsIC 2001 Oct. 2001, Baltimore,
MD
2
Outline
UCSB
GaAs IC 2001
  • Introduction
  • Ultra-low parasitic InP HBT technology
  • Circuit design
  • Results
  • Conclusion

3
G-band Electronics (140-220 GHz)
  • Applications
  • Wideband communication systems
  • Atmospheric sensing
  • Automotive radar
  • Transistor-based ICs realized through submicron
    device scaling
  • State-of-the-art InP-based HEMT Amplifiers with
    submicron gate lengths
  • 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.
  • HBT is a vertical-transport device (vs.
    lateral-transport) Presents Challenges to
    Scaling

4
Transferred-Substrate HBTs
  • Substrate transfer allows simultaneous scaling
    of emitter and collector widths
  • Maximum frequency of oscillation
  • Submicron scaling of emitter and collector
    widths has resulted in record values of measured
    transistor power gains (U20 dB at 110
    GHz)
  • Promising technology for ultra-high frequency
    tuned circuit applications
  • This Work
  • Single-stage tuned amplifier with 6.3 dB gain
    at 175 GHz
  • Gain-per-stage amongst highest reported in this
    band

Mesa HBT
Transferred-substrate HBT
5
InAlAs/InGaAs HBT Material System
Layer Structure
Band Diagram
2kT base bandgap grading
Bias conditions for the band diagram Vbe 0.7 V,
Vce 0.9 V
6
Transferred-Substrate Process Flow
  • 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

7
Ultra-high fmax Submicron HBTs
  • Electron beam lithography used to define
    submicron emitter and collector stripes
  • Minimum feature sizes
  • 0.2 ?m emitter widths
  • 0.3 ?m collector widths
  • Amplifier device dimensions
  • Emitter area 0.4 x 6 ?m2
  • Collector area 0.7 x 6.4 ?m2
  • Aggressive scaling of transistor dimensions
    predicts progressive improvement of fmax
  • As we scale HBT to lt0.4 um, fmax keeps
    increasing, devicemeasurements become very
    difficult

0.3 ?m Emitter before polyimide planarization
Submicron Collector Stripes(typical 0.7 um
collector)
8
Device Measurements
RF Gains
  • RF Measurements
  • Unilateral power gain shows peaking in DC-45 GHz
    band
  • 75-110 GHz measurements corrupted by excessive
    probe-to-probe coupling
  • Recent device measurements have shown negative
    unilateral power gain in W- and G- bands (2001
    DRC, Notre Dame)
  • Second-order device physics may be important in
    ultra-low parasitic devices
  • Implications
  • Devices have extremely high power gains in
    140-220 GHz bands, but fmax cannot be determined
    from 20 dB/decade extrapolation
  • Bias Conditions VCE 1.2 V, IC 4.8 mA
  • Device dimensions
  • Emitter area 0.4 x 6 ?m2
  • Collector area 0.7 x 6.4 ?m2
  • f? 160 GHz
  • DC properties ? 20, BVCEO 1.5 V

9
Amplifier Design
  • Simple common-emitter design conjugately matched
    at 200 GHz
  • 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
  • Shunt R-C network at output provides low
    frequency stabilization

S21
S11, S22
Schematic
10
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

11
140-220 GHz VNA Measurements
  • HP8510C VNA with Oleson Microwave Lab mmwave
    Extenders
  • GGB Industries coplanar wafer probes with WR-5
    waveguide connectors
  • Full-two port T/R measurement capability
  • Line-Reflect-Line calibration with on-wafer
    standards
  • Internal bias Tees in probes for biasing active
    devices

UCSB 140-220 GHz VNA Measurement Set-up
12
Amplifier Measurements
  • Measured 6.3 dB peak gain at 175 GHz
  • Device dimensions
  • Emitter area 0.4 x 6 ?m2
  • Collector area 0.7 x 6.4 ?m2
  • Device bias conditions
  • Ic 4.8 mA, VCE 1.2 V

S21
Cell Dimensions 690?m x 350 ?m
13
Simulation vs. Measurement
  • Amplifier designed for 200 GHz
  • Peak gain measured at 175 GHz
  • Possible sources for discrepancy
  • Matching network design
  • Device model

14
Matching Network Design
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
  • Simulation shows 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
15
Device Modeling I Hybrid-Pi Model
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

16
Device Modeling II Model vs. Measurement
  • Measurements and simulations of device 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

S21
S12
S11, S22
17
Simulation vs. Measurement
Simulation versus Measured Results Simulation
Using Measured Device S-parameters
  • Simulated amplifier using measured device
    S-parameters in the 140-220 GHz band
  • Simulation shows good 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

18
Multi-stage Amplifier Design
Simulation Results
  • Three-stage amplifier designed using measured
    transistor S-parameters
  • Simulated 20 dB gain at 175 GHz
  • Design currently being fabricated

Multi-stage amplifier layout
19
Conclusions
UCSB
GaAs IC 2001
  • Single-stage HBT amplifier with 6.3 dB at 175 GHz
  • 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
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