III-V Channel Transistors Jess A. del Alamo Professor Microsystems - - PowerPoint PPT Presentation

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III-V Channel Transistors Jess A. del Alamo Professor Microsystems - - PowerPoint PPT Presentation

III-V Channel Transistors Jess A. del Alamo Professor Microsystems Technology Laboratories MIT Acknowledgements: Students and collaborators: D. Antoniadis, J. Lin, W. Lu, A. Vardi, X. Zhao Sponsors: Applied Materials, DTRA, KIST,


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SLIDE 1

III-V Channel Transistors

Jesús A. del Alamo Professor Microsystems Technology Laboratories MIT

24 April 2017 Acknowledgements:

  • Students and collaborators: D. Antoniadis, J. Lin, W. Lu, A. Vardi, X. Zhao
  • Sponsors: Applied Materials, DTRA, KIST, Lam Research, Northrop Grumman,

NSF, Samsung

  • Labs at MIT: MTL, EBL
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SLIDE 2

Moore’s Law at 50: the end in sight?

2

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SLIDE 3

Moore’s Law

Moore’s Law = exponential increase in transistor density

3

Intel microprocessors

2016: Intel 22-core Xeon Broadwell-E5 7.2B transistors

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SLIDE 4

Moore’s Law

4

?

How far can Si support Moore’s Law?

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SLIDE 5

Transistor scaling  Voltage scaling  Performance suffers

5

Transistor current density:

Goals:

  • Reduced footprint with moderate short-channel effects
  • High performance at low voltage

Intel microprocessors Intel microprocessors

Supply voltage:

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SLIDE 6

6

Moore’s Law: it’s all about MOSFET scaling

  • 1. New device structures with improved scalability:
  • 2. New materials with improved transport characteristics:

n-channel: Si  Strained Si  SiGe  InGaAs p-channel: Si  Strained Si  SiGe  Ge  InGaSb

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SLIDE 7

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III-V electronics in your pocket!

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SLIDE 8

Contents

8

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SLIDE 9
  • 1. Self-aligned Planar InGaAs MOSFETs

9

Lin, IEDM 2012, 2013, 2014 W Mo Lee, EDL 2014; Huang, IEDM 2014 selective MOCVD Sun, IEDM 2013, 2014 Chang, IEDM 2013 reacted NiInAs dry-etched recess implanted Si + selective epi

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SLIDE 10

Self-aligned Planar InGaAs MOSFETs @ MIT

10

Lin, IEDM 2012, 2013, 2014

Recess-gate process:

  • CMOS-compatible
  • Refractory ohmic contacts
  • Extensive use of RIE

W Mo

0.0 0.1 0.2 0.3 0.4 0.5 0.0 0.2 0.4 0.6 0.8 1.0

Lg=20 nm Ron=224 m 0.4 V

Id (mA/m) Vds (V)

Vgs-Vt= 0.5 V

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SLIDE 11
  • Ohmic contact first, gate last
  • Precise control of vertical (~1 nm), lateral (~5 nm) dimensions
  • MOS interface exposed late in process

Fabrication process

11

W/Mo n+ InGaAs/InP InGaAs/InAs InAlAs SiO2 InP -Si Resist Mo Pad HfO2

Mo/W ohmic contact + SiO2 hardmask SF6, CF4 anisotropic RIE CF4:O2 isotropic RIE Cl2:N2 anisotropic RIE Digital etch

Waldron, IEDM 2007

Finished device

Lin, EDL 2014

O2 plasma H2SO4

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SLIDE 12
  • Channel: In0.7Ga0.3As/InAs/In0.7Ga0.3As (tch=9 nm)
  • Gate oxide: HfO2 (2.5 nm, EOT~ 0.5 nm)

Highest performance InGaAs MOSFET

12

Lg=70 nm:

  • Record gm,max = 3.45 mS/µm at Vds= 0.5 V
  • Ron = 190 Ω.µm

Lin, EDL 2016

3.45 mS/m

Exceeds best HEMT!

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SLIDE 13

Excess OFF-state current

13

OFF-state current enhanced with Vds  Band-to-Band Tunneling (BTBT) or Gate-Induced Drain Leakage (GIDL)

Lin, IEDM 2013

  • 0.6 -0.4 -0.2 0.0

10

  • 11

10

  • 9

10

  • 7

10

  • 5

Lg=500 nm Vds=0.3~0.7 V step=50 mV

Id(A/m) Vgs (V)

Transistor fails to turn off:

Vds ↑

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SLIDE 14
  • 0.4 -0.2 0.0 0.2

10

  • 11

10

  • 9

10

  • 7

10

  • 5

W/ BTBT+BJT W/O BTBT Vds=0.3~0.7 V step=50 mV

Id (A/m) Vgs (V)

Excess OFF-state current

14

Lg↓  OFF-state current ↑  bipolar gain effect due to floating body

Lin, EDL 2014

  • 0.6 -0.4 -0.2 0.0

10

  • 11

10

  • 9

10

  • 7

10

  • 5

Lg=500 nm Vds=0.3~0.7 V step=50 mV

Id(A/m) Vgs (V)

  • 0.6 -0.4 -0.2 0.0

10

  • 8

10

  • 7

10

  • 6

10

  • 5

10

  • 4

500 nm 280 nm 120 nm T=200 K Vds=0.7 V

Id (A/m) Vgs-Vt (V)

Lg=80 nm

Vds ↑

Simulations

w/ BTBT+BJT w/o BTBT+BJT

Lg=500 nm

Lin, TED 2015

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SLIDE 15
  • 2. InGaAs FinFETs

15

Intel Si Trigate MOSFETs

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SLIDE 16

Bottom-up InGaAs FinFETs

16

Si

Waldron, VLSI Tech 2014 Aspect-Ratio Trapping Fiorenza, ECST 2010 Epi-grown fin inside trench

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SLIDE 17

Top-down InGaAs FinFETs

17

Kim, IEDM 2013

60 nm

dry-etched fins Radosavljevic, IEDM 2010

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SLIDE 18

20 40 60 0.0 0.5 1.0 1.5 2.0

1.8 1 0.8 0.57

InGaAs FinFETs

5.3 4.3

Si FinFETs

gm[mS/m] Wf [nm]

0.63 0.6 0.23 0.66 1 0.18

FinFET benchmarking

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gm normalized by width of gate periphery

  • State-of-the-art Si FinFETs: Wf=7 nm

Natarajan, IEDM 2014

channel aspect ratio

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SLIDE 19

20 40 60 0.0 0.5 1.0 1.5 2.0

1.8 1 0.8 0.57

InGaAs FinFETs

5.3 4.3

Si FinFETs

gm[mS/m] Wf [nm]

0.63 0.6 0.23 0.66 1 0.18

19

Thathachary, VLSI 2015

gm normalized by width of gate periphery

  • Narrowest InGaAs FinFET fin: Wf=15 nm
  • Best channel aspect ratio of InGaAs FinFET: 1.8
  • gm much lower than planar InGaAs MOSFETs

Oxland, EDL 2016 Radosavljevic, IEDM 2011 Kim, IEDM 2013 Natarajan, IEDM 2014

channel aspect ratio

FinFET benchmarking

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SLIDE 20

InGaAs FinFETs @ MIT

20

Vardi, DRC 2014, EDL 2015, IEDM 2015

Key enabling technologies: BCl3/SiCl4/Ar RIE + digital etch

  • Sub-10 nm fin width
  • Aspect ratio > 20
  • Vertical sidewalls
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SLIDE 21

InGaAs FinFETs @ MIT

21

Vardi, VLSI Tech 2016 Vardi, EDL 2016

  • CMOS compatible process
  • Mo contact-first process
  • Fin etch mask left in place  double-gate MOSFET

InAlAs InGaAs

n+‐InGaAs

W/Mo Lg SiO2 HSQ High‐K InP δ ‐ Si InP Mo Mo HSQ High‐K InGaAs

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SLIDE 22

22

Most aggressively scaled FinFET

Wf=7 nm, Lg=30 nm, Hc=40 nm (AR=5.7), EOT=0.6 nm: Vardi, EDL 2016 At VDS=0.5 V:

  • gm=900 µS/µm
  • Ron=320 Ω.µm
  • Ssat=100 mV/dec
  • 0.4
  • 0.2

0.0 0.2 0.4 200 400 600 800 1000 VDS=0.5 V

gm max=900 S/m

gm [S/m] VGS [V]

  • 0.5 -0.4 -0.3 -0.2 -0.1 0.0

0.1 0.2 0.3 0.4 1E-9 1E-8 1E-7 1E-6 1E-5 1E-4 1E-3

VDS=50 mV DIBL=90 mV/V

Id [A/m] VGS [V]

Ssat=100 mV/dev VDS=500 mV

0.0 0.1 0.2 0.3 0.4 0.5 100 200 300 400 500 Id [A/m]

VDS [V] VGS=-0.5 to 0.75 VGS=0.25 V

Current normalized by 2xHc

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SLIDE 23

23

100 200 300 400 500 600 700

  • 0.6
  • 0.4
  • 0.2

0.0 0.2 0.4

EOT

VT [V] Lg [nm] 100 200 300 400 500 600 700 50 100 150 200 250 A: Al2O3, EOT=2.8 nm B:Al2O3/HfO2, EOT=1 nm C: HfO2, EOT=0.6 nm Ssat [mV/dec] Lg [nm]

EOT

60 mV/dec 100 200 300 400 500 600 700 200 400 600 800 1000 1200 1400 1600

EOT

VDS=0.5 V Wf20-22 nm

gm [S/m] Lg [nm] 100 200 300 400 500 600 700 50 100 150 200 250 300 350

EOT

Ioff=100 nA/m VDS=0.5 V Ion [A/m] Lg [nm]

Classical scaling with Lg and EOT

Lg and EOT scaling

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SLIDE 24

100 1000 50 100 150

Wf=7 nm Wf=12 nm Wf=17 nm Wf=22 nm

Ssat,min [mV/dec] Lg [nm] 60 mV/dec

Fin width scaling (EOT=0.6 nm)

24

  • Non-ideal fin width scaling
  • High Dit (~5x1012 cm-2.eV-1); mobility degradation; line edge roughness

Contaminated by gate leakage

100 200 300 500 1000 1500 2000 2500 12 17 Wf=22 nm Ron [m] Lg [nm] 7 nm 50 100 150 200 250 300

  • 0.3
  • 0.2
  • 0.1

0.0 0.1 0.2 0.3

 Wf=22 nm Wf= 5 nm

VT [V] Lg [nm] 100 200 300 400 500 600 200 400 600 800 1000 1200 1400 1600  Wf= 5 nm gm max [S/m] Lg [nm] Wf=22nm

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SLIDE 25

InGaAs FinFETs: gm benchmarking

25

gm normalized by width of gate periphery:

  • First InGaAs FinFETs with Wf<10 nm
  • Record results for InGaAs FinFETs with Wf < 25 nm
  • Still short of Si FinFETs (though they operate at VDD=0.8 V)

Hc Wf Hc

Double gate Trigate

20 40 60 0.0 0.5 1.0 1.5 2.0

1.8 1 0.8 0.57 5.7 3.3 2.31.8

InGaAs FinFETs

5.3 4.3

Si FinFETs

gm[mS/m] Wf [nm]

0.63 0.6 0.23 0.66 1 0.18

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SLIDE 26

InGaAs FinFETs: gm benchmarking

26

gm normalized by fin width (FOM for density): Doubled gm/Wf over earlier InGaAs FinFETs

Vardi, EDL 2016

Hc Wf Wf Hc

20 40 60 5 10 15 20

1 1.8 0.57 0.8 5.7 3.3 2.31.8

InGaAs FinFETs

5.3 4.3

Si FinFETs (VDD=0.8 V)

gm/Wf [mS/m] Wf [nm]

0.63 0.6 0.23 0.66 1 0.18

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SLIDE 27

Impact of fin width on VT

27

  • Strong VT sensitivity for Wf < 10 nm; much worse than Si
  • Due to quantum effects
  • Big concern for future manufacturing

InGaAs doped-channel FinFETs: 50 nm thick, ND~1018 cm-3

Vardi, IEDM 2015

T=90K

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SLIDE 28

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  • 3. Vertical nanowire MOSFET:

ultimate scalable transistor

Vertical NW MOSFET:  uncouples footprint scaling from Lg, Lspacer, and Lc scaling Lc Lg Lspacer

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SLIDE 29

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Vertical nanowire MOSFET for 5 nm node

Yakimets, TED 2015 Bao, ESSDERC 2014

Vertical NW:  power, performance and area gains w.r.t. Lateral NW or FinFET

5 nm node 30% area reduction in 6T‐SRAM 19% area reduction in 32 bit multiplier

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SLIDE 30

InGaAs Vertical Nanowires on Si by direct growth

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Björk, JCG 2012 Selective-Area Epitaxy Au seed Vapor-Solid-Liquid (VLS) Technique InAs NWs on Si by SAE Riel, MRS Bull 2014

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SLIDE 31

31

InGaAs VNW MOSFETs by top-down approach @ MIT

  • Sub-20 nm NW diameter
  • Aspect ratio > 10
  • Smooth sidewalls

Zhao, EDL 2014 Key enabling technologies:

  • RIE = BCl3/SiCl4/Ar chemistry
  • Digital Etch (DE) =

O2 plasma oxidation H2SO4 oxide removal

15 nm 240 nm

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SLIDE 32

InGaAs VNW Mechanical Stability for D<10 nm

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8 nm InGaAs VNWs: Yield = 0%

Broken NW

Difficult to reach 10 nm VNW diameter due to breakage

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SLIDE 33

InGaAs VNW Mechanical Stability for D<10 nm

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8 nm InGaAs VNWs: Yield = 0%

Broken NW

Difficult to reach 10 nm VNW diameter due to breakage Water-based acid is problem:

Surface tension (mN/m):

  • Water: 72
  • Methanol: 22
  • IPA: 23

Solution: alcohol-based digital etch

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SLIDE 34

Alcohol-Based Digital Etch

34

10% HCl in IPA Yield = 97% 10% HCl in DI water Yield = 0%

Alcohol-based DE enables D < 10 nm

Broken NW

Radial etch rate: 1.0 nm/cycle Radial etch rate: 1.0 nm/cycle

8 nm InGaAs VNWs Lu, EDL 2017

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SLIDE 35

InGaAs Digital Etch

35

First demonstration of D=5 nm diameter InGaAs VNW (Aspect Ratio > 40) Lu, EDL 2017

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SLIDE 36

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InGaAs VNW-MOSFETs by top-down approach @ MIT

Top-down approach: flexible and manufacturable

n+ InGaAs, 70 nm i InGaAs, 80 nm n+ InGaAs, 300 nm

Starting heterostructure: n+: 6×1019 cm‐3 Si doping

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SLIDE 37

Process flow

Tomioka, Nature 2012 Persson, DRC 2012 Zhao, IEDM 2013

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SLIDE 38

NW-MOSFET I-V characteristics: D=40 nm

38

Single nanowire MOSFET:

  • Lch= 80 nm
  • 3 nm Al2O3 (EOT = 1.5 nm)
  • gm,pk=720 μS/μm @ VDS=0.5 V
  • Slin=70 mV/dec, Ssat=80 mV/dec
  • DIBL=88 mV/V
  • 0.2

0.0 0.2 0.4 0.6 10

  • 10

10

  • 9

10

  • 8

10

  • 7

10

  • 6

10

  • 5

10

  • 4

10

  • 3

Vds=0.5 V

Vgs(V) Is (A/m)

Vds=0.05 V

0.0 0.1 0.2 0.3 0.4 0.5 50 100 150 200 250 300

Vgs=-0.2 V to 0.7 V in 0.1 V step

Vds (V)

Is A/m)

  • 0.2

0.0 0.2 0.4 0.6 100 200 300 400 500 600 700 800 Vgs(V) gm (S/m) Vd= 0.5 V

gm,pk=720 μS/μm

Slin = 70 mV/dec Ssat = 80 mV/dec DIBL = 88 mV/V

Zhao, CSW 2017

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SLIDE 39

200 400 600 200 400 600 800 1000 1200 1400 Vds=0.5 V

Ssat (mV/dec)

gm,pk (S/m)

Tanaka, APEX 2010

Tomioka, IEDM 2011

Tomioka, Nature 2012 Persson, DRC 2012 Persson, EDL 2010

Zhao, IEDM 2013

Berg, IEDM 2015 This work

Top‐down VNW‐MOSFETs as good as bottom up devices

39

Persson, DRC 2012 Tomioka, Nature 2012 Tanaka, APEX 2010 Berg, IEDM 2015

InGaAs VNW-MOSFETs Benchmark

This work

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SLIDE 40

How are we doing in terms of short-channel effects?

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del Alamo, J-EDS 2016 Slin: linear subthreshold swing Lg= gate length λc= electrostatic scaling length: f(tox, tch) Ideal scaling

FinFET Planar-MOSFET VNW MOSFET

  • Reasonable scaling behavior but…
  • Excessive Dit
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SLIDE 41
  • 4. InGaSb p–type MOSFETs

41

Nainani, IEDM 2010

Planar InGaSb MOSFET demonstrations:

Takei, Nano Lett. 2012

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SLIDE 42

InGaSb p–type FinFETs @ MIT

42

Lu, IEDM 2015

Key enabling technology:

  • BCl3/N2 RIE
  • [digital etch under development]

15 nm fins, AR>13 20 nm fins, 20 nm spacing

  • Smallest Wf = 15 nm
  • Aspect ratio >10
  • Fin angle > 85°
  • Dense fin patterns
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SLIDE 43

Si-compatible contacts to p+-InAs

43

Lu, IEDM 2015

Ni/Ti/Pt/Al on p+-InAs (circular TLMs): Record ρc: 3.5x10-8 Ω.cm2 at 400oC

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SLIDE 44

InGaSb p-type FinFETs

44

Lu, IEDM 2015

  • Fin etch mask left in place  double-gate MOSFET
  • Channel: 10 nm In0.27Ga0.73Sb (compressively strained)
  • Gate oxide: 4 nm Al2O3 (EOT=1.8 nm)
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SLIDE 45
  • First InGaSb FinFET
  • Peak gm approaches best InGaSb planar MOSFETs
  • Poor turn off

InGaSb FinFET I-V characteristics

45

  • Lg = 100 nm, Wf = 30 nm (AR=0.33)
  • Normalized by conducting gate periphery

Lu, IEDM 2015

0.01 0.1 1 10 100 10 100

Yuan, 2013 [7] Nainani, 2010 [8] Chu, 2014 [11] Xu, 2011 [12] Nagaiah, 2011 [13]

In0.36Ga0.64Sb GaSb

gm (S/m) Lg (m)

This work (FinFET) In0.27Ga0.73Sb GaSb In0.35Ga0.65Sb In0.2Ga0.8Sb

Planar MOSFETs

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SLIDE 46

InGaSb p-Channel FinFETs (2nd gen.)

46

Vd(V)

  • 1
  • 0.8
  • 0.6
  • 0.4
  • 0.2

50 100 150 200

Vg: 1 to -1.6 in -0.4V step, Rtot:2.30e+03

  • m
  • Lg = 100 nm, Wf = 18 nm (AR=0.42)
  • Channel: 7.5 nm In0.4Ga0.6Sb
  • gm,max = 200 µS/µm
  • Still poor turn-off  need digital etch, better sidewall passivation

0.01 0.1 1 10 100 10 100

Gen 2 In0.4Ga0.6Sb Gen 1 In0.2Ga0.8Sb Yuan, 2013 Nainani, 2010 Chu, 2014 Xu, 2011 Nagaiah, 2011

In0.36Ga0.64Sb GaSb

gm (S/m) Lg (m)

Gen 1 In0.27Ga0.73Sb

GaSb In0.35Ga0.65Sb In0.2Ga0.8Sb

Planar MOSFETs

Lu, CSW 2017

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SLIDE 47
  • 5. Co-integration of SiGe p-MOSFETs

and InGaAs MOSFETs on SOI

47

InGaAs n-MOSFET

Czornomaz, VLSI Tech 2016

SiGe p-MOSFET 6T-SRAM

SiGe InGaAs Si SiO2

Confined Epitaxial Lateral Overgrowth

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SLIDE 48

Conclusions

1. Great recent progress on planar, fin and nanowire InGaAs MOSFETs 2. Device performance still lacking for multigate designs 3. P-type InGaSb MOSFETs in their infancy 4. Many, MANY issues to work out:

sub-10 nm fin/nanowire fabrication, self-aligned contacts, device asymmetry, introduction of mechanical stress, VT control, sidewall roughness, device variability, BTBT and parasitic HBT gain, trapping, self- heating, reliability, NW survivability, co-integration on n- and p-channel devices on Si, …

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SLIDE 49

Hype curve for III-V CMOS?

# Papers on III-V CMOS at IEDM Year

49

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SLIDE 50

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A lot of work ahead but… exciting future for III-V electronics

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SLIDE 51