Title: 87 GHz Static Frequency Divider in an InPbased Mesa DHBT Technology
187 GHz Static Frequency Divider in an InP-based
Mesa DHBT Technology
- S. Krishnan, Z. Griffith, M. Urteaga, Y. Wei,
- D. Scott, M. Dahlstrom, N. Parthasarathy and M.
Rodwell - Department of Electrical and Computer
Engineering, - University of California, Santa Barbara
griffith_at_ece.ucsb.edu 805-893-8044
GaAsIC, October 2002Monterey, CA
2Why Static Frequency Dividers (SFD)?
MS flip-flops are very widely-used high speed
digital circuits Master-Slave Flip-Flop with
inverting feedback Connection as 21
frequency divider provides simple test method
Standard benchmark of logic speed
Performance comparisons across
technologies Dynamic, super-dynamic, frequency
dividers Higher maximum frequency than
true static dividers Narrow-band operation
? more limited applications High Speed
technology performance HRL gt 100 GHz
dividerthis conference with E2CL UCSB 75 GHz
static dividers using InAlAs/InGaAs TS-HBTs HRL
72.8 GHz static dividers using InAlAs/InGaAs HBTs
3Why Static Dividers, and what makes them fast
MS latch key digital element resynchronizes
data to clock often sets system maximum clock
- f? does not predict logic speed
- fmax does not predict logic speed
-
- Large signal operation involves switching time
constants ??
4Mesa DHBT Epitaxial Layer Structure
InP Emitter n doped
P InGaAs Base 52 meV Band gap grading
2000 Å n- InP Collector
5mesaIC Process Key Features
Slide 1
6mesaIC Process Key Features
Slide 2
7mesaIC Process Key Features
Slide 3
8mesaIC Process Key Features
Slide 4
9mesaIC Process Key Features
Slide 5
10mesaIC Process Key Features
Slide 6
11mesaIC Process Key Features
Slide 7
12mesaIC Process Key Features
Slide 8
13mesaIC Process Key Features
Slide 9
14mesaIC Process Key Features
Slide complete
15mesaIC Process overview
- Both junctions defined by selective wet-etch
chemistry - Narrow base mesa allows for low
- AC to AE ratio
- Low base contact resistance
- Pd based ohmics with ?C lt 10-7 ?cm2
- Collector contact metal and metal 1 used as
interconnect metal - NiCr thin film resistors 40 ? / ?
- MIM capacitor, with SiN dielectric -- used
only for bypass capacitors - Low loss, low ?r 2.7 microstrip wiring
environment
- Microstrip wiring environment.
- has predictable characteristic impedance
- controlled-impedance interconnects within
dense mixed signal ICs - ground plane eliminates signal coupling that
occurs through on-wafer gnd-return inductance
16DC and RF measurements
- Common emitter characteristics
- Device geometry emitter metal 0.7 ? 8.0
?m2, real device 0.6 7.0 ?m2 - Collector to emitter area ratio, AC / AE 4.5
- IB 50 ?A per step
- DC beta ? 20
- Self heating presentnot observed
- in previous runs with same material
- f? 205 GHz, fmax 210 GHz
- Measurement condition
- VCE 1.2 Volts, Jc 2.5 mA/?m2
17Circuit diagram Static Frequency Divider
- Circuit Details.
- ECL topology
- JEF 2.0 mA / ?m2
- Jsteering 2.5 mA / ?m2
- VEE - 4.5 Volts
- Microstrip interconnects
- Output voltage for acquire and hold
components, ?V 300mV - Output buffer used for measurement isolation,
Vout ? 300 mV
Hold ckt
Acquire ckt
18Chip Photograph 87 GHz Divider
19Measurements DC 40 GHz setup
? 0 d?m
Sampling oscilloscope
DC - 40 GHz Synthesizer
Clk
Out
VEE
- Clock input ? 0 d?m
- Divider Operation from 4 GHz to 40 GHz
- Measurement establishes fully static nature of
divider
Output waveform _at_ 2 GHz fclk 4 GHz
20Measurements 50 75 GHz setup
- Clock input ? 0 d?m
- Divider Operation from 50 GHz to 75 GHz
Output waveform _at_ 37.5 GHz fclk 75 GHz
21Measurements 75 110 GHz setup
Sampling oscilloscope
? 9.7 d?m
Out
Clk
VEE
- Clock input ? 9.7 d?m
- Divider Operation from 75 GHz to 87 GHz
Output waveform _at_ 43.5 GHz fclk 87 GHz
22Conclusions
- Accomplishments
- Demonstrated a fully static, static frequency
divider in a narrow triple-mesa DHBT processup
to 87 GHz - Future Direction
- Reduce device parasitics (rex, rbb) and wiring
capacitance - Increased current density (JE) reduces
-
- Continued lateral scaling of base contact to
decrease - AE / AC ratio lower CCB
- Acknowledgements
- This work was support by the Office of Naval
Research (ONR--N00014-01-1-0024) and by Walsin
Lihwa / UC Core