Si CMOS for RF Power Applications J. A. del Alamo MIT Workshop on - - PowerPoint PPT Presentation

si cmos for rf power applications
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Si CMOS for RF Power Applications J. A. del Alamo MIT Workshop on - - PowerPoint PPT Presentation

Si CMOS for RF Power Applications J. A. del Alamo MIT Workshop on Advanced Technologies for Next Generation of RFIC 2005 RFIC Symposium June 12, 2005 Sponsors: DARPA, IBM, SRC RF power applications Power vs. frequency GaAs HEMT 50 InP


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SLIDE 1

Si CMOS for RF Power Applications

  • J. A. del Alamo

MIT

Workshop on Advanced Technologies for Next Generation of RFIC 2005 RFIC Symposium June 12, 2005 Sponsors: DARPA, IBM, SRC

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SLIDE 2

RF power applications

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SLIDE 3

10 20 30 40 50 0.1 1 10 100 1000 Frequency [GHz] Output Power [dBm]

GaAs HEMT InP HEMT Si BJT SiGe HBT GaAs / InP HBT GaAs MESFET GaN HEMT LDMOS CMOS

Power vs. frequency

Compilation of research papers from IEEE Xplore by J. Scholvin

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SLIDE 4

Research activity by material and frequency

Compilation of research papers from IEEE Xplore by J. Scholvin

25 50 75 100 1985 1987 1989 1991 1993 1995 1997 1999 2001 2003 Year Publications per Year SiC InP GaN GaAs Silicon 25 50 75 100 1985 1987 1989 1991 1993 1995 1997 1999 2001 2003 Year Publications per Year above 27 GHz 3 to 27 GHz below 3 GHz

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SLIDE 5

RF power technologies: 1993 vs. 2003

Compilation of research papers from IEEE Xplore by J. Scholvin

GaAs MESFET 34% InP HEMT 12% GaAs HBT 12% GaAs HEMT 37% LDMOS 5%

1993 2003

SiC 3% GaAs MESFET 5% GaN HEMT 16% InP HBT 3% InP HEMT 3% GaAs HBT 16% GaAs HEMT 22% CMOS 16% LDMOS 5% Si BJT 3% SiGe HBT 10% Silicon 34%

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SLIDE 6

RF Power Figures of Merit

  • PA specs:

– Frequency

– Power – Gain – Linearity – Voltage – Reliability – Power efficiency – Cost PA

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SLIDE 7

Fundamental trade-off between voltage and frequency

scaling

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SLIDE 8

Key to power: supply voltage

0.0001 0.001 0.01 0.1 1 10 100 0.1 1 10 100

Vdd [V] Power Density [W/mm]

GaN HEMT GaAs & InP HBT LDMOS CMOS GaAs MESFET HEMT Si BJT SiGe HBT

Compilation of research papers from IEEE Xplore by J. Scholvin

Wf

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SLIDE 9

20 40 60 80 100 0.1 1 10 100 1000 Frequency [GHz] Power Added Efficiency [%]

GaAs/InP HBT InP HEMT GaAs HEMT GaAs MESFET CMOS SiGe HBT LDMOS

Key to frequency: efficiency

Compilation of research papers from IEEE Xplore by J. Scholvin

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SLIDE 10

The benefits of scaling

20 40 60 0.2 0.4 0.6 0.8 1 Lg [µm] Peak PAE [%]

All FETs 27 GHz < f < 50 GHz

Compilation of research papers from IEEE Xplore by J. Scholvin

scaling scaling

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SLIDE 11

Si CMOS: a disruptive technology for RF power?

0.01 0.1 1 10 1970 1980 1990 2000 2010 Year Physical Gate Length [µm]

III-V's CMOS CMOS Roadmap

Gate length scaling in III-V FETs and CMOS

Compilation of research papers from IEEE Xplore by J. Scholvin

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SLIDE 12

Si MOSFETs for RF power

10 20 30 40 50 0.1 1 10 100 1000 Frequency [GHz] Output Power [dBm]

GaAs HEMT InP HEMT Si BJT SiGe HBT GaAs / InP HBT GaAs MESFET GaN HEMT LDMOS CMOS

  • 1. Extending LDMOS beyond 2 GHz
  • 2. RF power suitability of deeply scaled CMOS
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SLIDE 13
  • 1. Extending LDMOS beyond 2 GHz

(PhD Thesis of J. Fiorenza)

Source Source

  • Two critical sources of RF Loss:

– Gate resistance loss: reduces power gain – Substrate loss: reduces power efficiency

Drain

Gate

Drain

Gate

LDMOSFET: Lightly-doped Drain MOSFET

n+ n-

n+ P

n+

Source Drain

n- Gate

n+ n-

n+ P

n+

Source Drain

n- Gate

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SLIDE 14

n-

300 nm 50 nm 50 nm Al TiN PolySi Gate Oxide 20 or 30 nm

n-

300 nm 50 nm 50 nm Al TiN PolySi Gate Oxide 20 or 30 nm

Low-loss gate: Metal/Poly-Si damascene gate

Advantages:

– Implemented in the back end of process

– Allows the use of Al or Cu: very low gate resistance – Self-aligned: no increase in overlap capacitance – Gate oxide undisturbed Achieved: 0.2 ohm/sqr (>10 for polySi, ~1 for silic’d gate)

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SLIDE 15

Metal/Poly-Si Damascene Gate

3 μm Source Gate Drain 200 μm

Lg = 0.6 μm ft ~ 15 GHz BVoff > 18 V

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SLIDE 16

0.6 μm minimum Lg 10 mask levels 2 levels of metal Fabricated at MIT

Test chip

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SLIDE 17

Benefit of low gate resistance: small signal

Damascene gate increases fmax, enables wide gate fingers

Source Source Drain Gate

Wf

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SLIDE 18

Benefit of low gate resistance: large signal

High PAE with gate finger width up to 140 μm

Source Source Drain Gate

Wf

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SLIDE 19

Low-loss substrates: SOI and high-resistivity Si

Substrate:

  • Regular Si
  • High-resistivity Si

Handle wafer:

  • Regular Si
  • High-resistivity Si

Drain

Gate

Drain

Gate n+ n-

n+ P

n+

Source Drain

n-

Gate

n+ n-

n+ P

n+

Source Drain

n-

Gate

Bulk Si Thin-film SOI

Drain

Gate

Drain

Gate n+ n-

n+ P

n+

Source Drain

n-

Gate

n+ n-

n+ P

n+

Source Drain

n-

Gate

n+ n-

n+ P

n+

Source Drain

n-

Gate

Bulk Si Thin-film SOI

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SLIDE 20

Impact of substrate

  • SOI improves PAE
  • High-resistivity silicon improves PAE on bulk
  • High-resistivity silicon does not improve PAE on SOI
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SLIDE 21

Beyond 2 GHz

Low-loss substrate very important at high frequencies

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SLIDE 22

Analysis of substrate loss

Gate Source

Drain Loss

Drain Pad

Pad Loss

  • Pad Loss:
  • SOI effective
  • HR effective on bulk Si and SOI
  • Drain Loss:
  • SOI somehow effective
  • HR very effective on bulk Si, only moderately on SOI
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SLIDE 23

Why is HRSOI Ineffective?

Drain Pad Gate Source HRSOI

  • - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -

Rsub Rsurf Cbox n+ p

n+

Surface inversion increases drain loss on HRSOI

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SLIDE 24

Effect of substrate inversion in HRSOI-LDMOS

30 35 40 45 50 55 60

  • 30
  • 20
  • 10

10 20 30 VHS [V] Peak PAE [%] 4.8 GHz 2.4 GHz

+

  • VHS

HRSOI RFin RFout Load-Pull Measurement

  • Eliminating substrate inversion improves PAE
  • Most prominent at high frequencies
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SLIDE 25

Impact of inversion layer elimination

45 50 55 60 Bulk HR Bulk SOI HR SOI Peak PAE [%]

Substrate Enhancement due to elimination of inversion layer

f=1.9 GHz

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SLIDE 26

Impact of inversion layer elimination

30 35 40 45 50 55 60 65 2 3 4 5 6 7 8 Frequency [GHz] peak PAE [%] VHS = 5.5 V VHS = 0 V

2 4 6 8 10 12 14

  • 10
  • 5

5 10 15 20 25 Output Power [dBm] Gain [dB] 10 20 30 40 50 60 PAE [%] f = 4.8 GHz 36x40 µm Vdd = 3.6 V Id = 10 mA

VHS=5.5 V VHS=0 V

  • Eliminating substrate surface effects improves performance:

– Particularly prominent in LDMOS due to large drain area – Both linear and saturated performance – Most prominent at high frequencies

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SLIDE 27

10 20 30 40 50 0.1 1 10 100 1000 Frequency [GHz] Output Power [dBm]

GaAs HEMT InP HEMT Si BJT SiGe HBT GaAs / InP HBT GaAs MESFET GaN HEMT LDMOS CMOS

Si MOSFETs for RF power

  • 1. Extending LDMOS beyond 2 GHz
  • 2. RF power suitability of deeply scaled CMOS
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SLIDE 28
  • 2. RF power suitability of deeply scaled CMOS

(PhD Thesis of J. Scholvin)

Attractiveness of CMOS:

  • System-on-Chip integration
  • Low cost
  • Low voltage
  • Good device models
  • Aggressive roadmap
  • Wide flavor of devices available

Suitable for:

  • High-volume, low cost consumer applications
  • Moderate frequencies (2-10 GHz)
  • Medium power (<100 mW)
  • Current: WLAN, Bluetooth, Cell-phone PA driver, WiMax/802.16

Picture from: http://www.intel.com/research/silicon/micron.htm#silicon

90 nm CMOS

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SLIDE 29
  • Concerns: CMOS scaling ⇒ Vdd ↓ ⇒ Pout ↓
  • Possible solutions:

– Raise Vdd ⇒ impact on reliability – Use I/O devices ⇒ not really scaling

Issues of CMOS for RF power

data for IEEE published CMOS PA devices and circuits

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SLIDE 30

90 nm CMOS: there is a lot more than 90 nm devices!

  • Includes devices with longer gate lengths and thicker

gate oxides for I/O drivers and high V operation

  • Designed RF power devices in collaboration with IBM

thick (51A) medium (22 A) thin (14 A) Oxide thickness 2.5 1.2 1.0 Nominal voltage [V] x x x Lg = 250 nm x x Lg = 130 nm x Lg = 90 nm

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SLIDE 31

The benefits of scaling for RF

  • Logic devices at optimized bias point have very high bandwidth
  • But… power devices at class AB bias point have much less bandwidth

50 100 150 200 90 nm 130 nm 250 nm

Device type fmax (GHz)

power device logic device

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SLIDE 32

RF power performance of standard 90 nm devices

Vdd = 1 V, Id = 26 mA/mm f = 2.2 GHz 48x16 µm (1 cell) 8 x 48x16 (8 cell)

  • 1 cell: Peak PAE = 66% at Pout = 12.5 dBm
  • 8 cell: Peak PAE = 59% at Pout = 20.2 dBm

10 20 30 40 50 60 70

  • 20
  • 10

10 20 30 Pout [dBm] Gain [dB], PAE [%] Gain PAE 1 cell 8 cells

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SLIDE 33

Linear performance of 90 nm CMOS

Vdd = 1 V Id = 26 mA/mm freq = 2.2 GHz 8x48x16 µm

  • What is PAE at a given IM3 ?

– at IM3 = -35 dBc, PAE = 12% at Pout = 12 dBm

  • Exceeds WCDMA PA driver specs

10 20 30 40 50 60 70

  • 20
  • 10

10 20 30 Pout [dBm] PAE [%]

  • 100
  • 80
  • 60
  • 40
  • 20

IM3 [dBc]

IM3 PAE WCDMA PA driver spec

  • 35 dBc
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SLIDE 34

90 nm vs. 250 nm devices at 8 GHz

  • At Vdd = 1 V, 90 nm has best PAE and Pout
  • 250 nm device offers highest power density at Vdd=2.5 V

10 20 30 40 50 60 70 0.1 1.0 10.0

Vdd [V] Peak PAE [%]

5 10 15 20 25 30

Output Power Density [dBm at 1 mm]

Lg = 90nm, Thin Ox Lg = 250nm, Thick Ox

Pout

freq = 8 GHz Id = 26 mA/mm

PAE

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SLIDE 35

90 nm vs. 250 nm

  • 250 nm thick oxide device has higher Vds,sat

⇒ compresses earlier and softer ⇒ lower Pout and peak PAE

  • As Vdd ↑ impact of Vds,sat decreases

90 nm, thin oxide 250 nm, thick oxide

Vgs = 1V Vgs = 2.4V 0.1V steps 0.2V steps

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SLIDE 36

What about reliability?

For RF power, reliability related to ratio of:

  • nominal Vdd
  • to breakdown voltage

For RF power:

  • 90 nm device expected to be more reliable at Vdd=1 V than

250 nm device at 2.5 V

1 2 3 4 5 6 90 nm 130 nm 250 nm

Device type BVoff, Vnom (V) Vnom BVoff

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SLIDE 37

Reliability: impact of output power

  • Run device under continuous RF power conditions
  • Measure drop in gain over time, define MTTF as 0.2 dB drop
  • Power compression has huge impact on degradation

Vdd = 1.6 V Id = 26 mA/mm f = 8 GHz 48x16 μm

20 40 60

  • 20
  • 10

10 Input Power [dBm] Gain [dB], PAE [%]

Gain PAE

  • 0.5
  • 0.4
  • 0.3
  • 0.2
  • 0.1

0.01 0.1 1 10 100 1000 Time [minutes] Change in Gain [dB]

Pout = 17.6 dBm 17.4 dBm 17.2 dBm 16.8 dBm

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SLIDE 38

Reliability: impact of Vdd

  • For same Vdd, thick oxide is more reliable

– but thin oxide has better performance

  • For identical lifetime, how does performance compare?

Impedances and RF power set for peak PAE Id = 26 mA/mm freq = 8 GHz

0.01 0.1 1 10 1 10 Vdd [V] Mean Time to Failure [hours] 90 nm thin oxide 250 nm thick oxide

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SLIDE 39

Reliability: impact of Vdd

Impedances and RF power set for peak PAE Id = 26 mA/mm freq = 8 GHz

0.01 0.1 1 10 1 10 Vdd [V] Mean Time to Failure [hours] 90 nm thin oxide 250 nm thick oxide

  • 90 nm thin ox. outperforms 250 nm thick ox. for high MTTF

– Low Vdd performance of 90 nm device much better than 250 nm device PAE=58%, Pout=16.8 dBm PAE=56%, Pout=15.6 dBm

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SLIDE 40

Conclusions

  • Metal-containing gates and low-loss substrates will

project LDMOS to 5-6 GHz

  • Deeply scaled CMOS suitable for RF power for:

– Moderate power levels (~100 mW) – Very low operating voltage (~1 V and below)

  • Scaling will project CMOS beyond 10 GHz
  • Si-based RF power technologies will dominate many

high-volume consumer applications: – WLANs, bluetooth, cellphone PA drivers, RF tags, etc

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SLIDE 41

MIT’s RF power measurement setup

– 1.8 - 18 GHz Maury ATS automatic load-pull system – 8-inch Cascade on-wafer probe station – Synthesized source with 10 W TWT-PA supplying up to 200 mW at DUT

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SLIDE 42

References

  • LDMOS:

– Bengtsson: MTT 2003 – Fiorenza: SOI Conf. 1999; MTT-S 2001; IEDM 2002, EDL 2001, 2003, 2005; TED 2002 – Scholvin: IEDM 2003 – Van der Heijden: MTT-S 2001

  • 90 nm CMOS:

– Ferndahl: MGWL 2003 – Scholvin: IEDM 2004