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60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles
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60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

Oct 08, 2019

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Page 1: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

60-GHz CMOS Transceivers: Why and How?

Behzad Razavi

Electrical Engineering Department

University of California, Los Angeles

Page 2: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

2

Outline

IntroductionReceiver Front EndTransmitter Front EndFrequency DividerReflectionsConclusion

Page 3: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

3

Why 60 GHz?

7 GHz of Unlicensed BandPossibility of Realizing (Multiple) On-Chip Antennas:- Low-Cost Packaging- Differential Operation Higher Output Power- No Need for T/R Switch- No Need for AC Coupling- No Need for High-Frequency ESD DevicesPossible Applications:- Gb/s Networks, e.g., Video Streaming- Highly-Interconnected Networks

Page 5: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

5

Why CMOS?

Need Complex Modulation Techniques:- OFDM- QAM- Frequency Hopping?Need Sophisticated Analog Calibration:- I/Q Matching at 60 GHz?!- Wideband Analog Baseband Filters- Multitude of High-Speed ADCsLarge Fractional Bandwidth (>10%):- Several Staggered High-Q Signal Paths- Multiple VCOs and Tuned Dividers

Page 6: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

6

Challenges

Limited transistor speed Need for inductors and transmission lines.Inductor footprints Long interconnectsInductor Q's tend to saturate around 25.Varactor Q's likely to be lower than inductor Q's.Lossy on-chip antennas BeamformingPassive and active device modelingGain and phase mismatches, etc.

Page 7: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

7

Transceiver Building Blocks

ReceiverFront End

Designed in 0.13-μm CMOS; migrating to 90-nm process.

JSSC, Jan.06 RFIC Symp, June 06

RFIC Symp, June 06

TransmitterFront End

FrequencyDivider

Page 8: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

8

Receiver Architecture

Balun

Page 9: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

9

Raw Speed of MOS Devices

Page 10: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

10

Coplanar Line Microstrip Line

Spiral Inductors vs. Transmission Lines

Page 11: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

11

Folded Microstrip

Page 12: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Choice of Linewidth

Page 13: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

13

S

A

A'

Choice of Line Spacing

Page 14: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

14

Choice of Line Spacing

Page 15: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

15

Cascode vs. Common-Gate LNA

Page 16: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Simplified LNA

Page 17: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Complete LNA

Page 18: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Mixer Design

Conventional Mixer Proposed Mixer

Page 19: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

19

On-Chip Balun

Page 20: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Receiver Floor Plan

Page 21: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

21

Input

LO

BB

Out

put

Active Area = 300 um x 400 um

Die Photograph

Page 22: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

22

Measured Performance

Page 23: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

23

3-dB improvement in SNR for twice the power consumption and area.

Other Thoughts

Page 24: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

24

Transmitter Front End

Slot Antenna- Large Area- High LossDipole- Narrow Footprint- Moderate Loss(~6 dB)

Page 25: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

25

Transmitter Design

Pout = -10 dBm

Psupp = 44 mW

Page 26: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Nested Inductors

Page 27: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Effect of Mutual Coupling

168170172174176178180182184186188

-0.4 -0.3 -0.2 -0.1 0 0.1 0.2 0.3 0.4

Mutual Coupling (k)

Out

put V

olta

ge (m

V)

Page 28: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

28

Die Photograph

Page 29: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Measurement Setup

Page 30: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

30

Antenna Radiation Pattern

Page 31: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

31

Flipflop-Based Dividers Miller DividerInjection-Locked Divider

Conventional Divider Topologies

Page 32: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Injection-Locked Divider

Narrow frequency range; inversely proportional to tank Q:

Page 33: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Phase noise degrades if, due to mismatches, input frequency is not equal to 2ω0.

Phase Noise Degradation

Page 34: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Increasing the Range

[Rategh et al, JSSC, May 00]

Ganged tuning does not overcome frequency

mismatch.

Difficult to guarantee natural frequency of divider

tracks that of VCO.

Page 35: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Tracking Issues

Page 36: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Phase-Locked Divider

Constant phase noise across range if gain of PD remains constant.No trade-off with tank Q. PD circuit must be very simple and experience complete switching.

Page 37: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Phase-Locked Divider

Page 38: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

38

Die Photograph

Page 39: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Measured Output

Page 40: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Phase Noise across Range

Page 41: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Divider

Challenges Revisited

LO (I/Q) GenerationLO DivisionLO Distribution

LNA I/Q Mixers

QuadratureVCO

Page 42: 60-GHz CMOS Transceivers: Why and How? - IEEE · 60-GHz CMOS Transceivers: Why and How? Behzad Razavi Electrical Engineering Department University of California, Los Angeles

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Conclusion

60-GHz transceivers can form highly-intercon-nected networks carrying high data rates. Nested inductors allow compact layout andshorter interconnects.Phase-locked dividers can provide a widefrequency range.Direct-conversion transceivers face difficultissues with respect to LO generation, division, and distribution.