Improved Regrowth of Self-Aligned Ohmic Contacts for III-V FETs North American Molecular Beam...

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3 Wistey, NAMBE 2009 Motivation for Regrowth: Scalable III-V FETs Classic III-V FET (details vary): Channel Bottom Barrier InAlAs Barrier Top Barrier or Oxide Gate Low doping Gap SourceDrain Large Rc { Large Area Contacts { III-V FET with Self-Aligned Regrowth: Channel In(Ga)P Etch Stop Bottom Barrier High-k Gate n+ Regrowth High Velocity Channel Implant: straggle, short channel effects Advantages of III-V’s Disadvantages of III-V’s Small R access Small Rc Self-aligned, no gaps High doping: cm -2 avoids source exhaustion 2D injection avoids source starvation Dopants active as-grown High mobility access regions High barrier Ultrathin 5nm doping layer }

Transcript of Improved Regrowth of Self-Aligned Ohmic Contacts for III-V FETs North American Molecular Beam...

Improved Regrowth of Self-Aligned Ohmic Contacts for III-V FETs

North American Molecular Beam Epitaxy Conference (NAMBE),8-11-2009

Mark A. Wistey

Now at University of Notre Damemwistey@nd.edu

mwistey@nd.edu

A.K. Baraskar, U. Singisetti, G.J. Burek, M.J.W. Rodwell, A.C. GossardUniversity of California Santa Barbara

P. McIntyre, B. Shin, E. KimStanford University

Funding: SRC

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Outline: Regrown III-V FET Contacts

•Motivation for Self-Aligned Regrowth

•Facets, Gaps, Arsenic Flux and MEE

•MOSFET Results•Conclusion

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Motivation for Regrowth: Scalable III-V FETs

Classic III-V FET (details vary):

ChannelBottom BarrierInAlAs Barrier

Top Barrier or Oxide

Gate

Low doping

GapSource Drain

Large Rc {

Large Area Contacts{III-V FET with Self-Aligned Regrowth:

ChannelIn(Ga)P Etch Stop

Bottom Barrier

High-k

Gate

n+ Regrowth

High Velocity Channel

Implant: straggle,short channel effects

• Advantages of III-V’s

• Disadvantages of III-V’s

Small Raccess

Small RcSelf-aligned, no gaps

High doping: 1013 cm-2 avoids source exhaustion

2D injection avoids source starvation

Dopants active as-grown

High mobilityaccess regions

High barrier

Ultrathin 5nm doping layer}

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MBE Regrowth: Bad at any Temperature?

• Low growth temperature (<400°C):

–Smooth in far field–Gap near gate (“shadowing”)–No contact to channel (bad)

Gate

200nm Gap

Source-DrainRegrowth

SEMs: Uttam Singisetti

Metals

Channel

SiO2

high-k Gate

Source-DrainRegrowth

Regrowth: 50nm InGaAs:Si, 5nm InAs:Si. Si=8E19/cm3, 20nm Mo, V/III=35, 0.5 µm/hr.

•High growth temperature (>490°C):– Selective/preferential epi on InGaAs– No gaps near gate

– Rough far field – High resistance

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560C

490C460C

SiO2 dummy

gate

SiO2 dummy

gate

540C

No gaps, but

faceting next to gates

Gap

High Temperature MEE: Smooth & No Gaps

Smooth

regrowth

Note faceting: surface kinetics, not shadowing.

In=9.7E-8, Ga=5.1E-8 Torr

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Shadowing and Facet Competition

[111]

[100]

Fast surface diffusion = slow facet

growth

Slow diffusion = rapid facet growth

Shen & Nishinaga, JCG 1995

[111] faster[100] faster

• Shen JCG 1995 says:Increased As favors [111] growth

SiO

2

[111]

[100]

Slow diffusion =fast growth

Fast surface diffusion =

slow facet growth

SiO

2

Good fill next to gate.

• But gap persists

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Gate Changes Local Kinetics

[100]

2. Local enrichment of III/V ratio

4. Low-angle planes grow insteadsidew

all

1. Excess In & Ga don’t stick to SiO2

• Diffusion of Group III’s away from gate

3. Increased surface mobility

Gate

SiO2 or SiNx

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Change of Faceting by Arsenic Flux

SiO2WCr

Increasing As flux

Original Interface

InAlAsmarkers

InGaAs

0.5x10-6

1x10-6

2x10-6

5x10-6

• Lowest arsenic flux → “rising tide fill”

• No gaps near gate or SiO2/SiNx

• Tunable facet competition

(Torr)

Growth conditions: MEE, 540*C, Ga+In BEP=1.5x10-7 Torr, InAlAs 500-540°C MBE.

• InGaAs layers with increasing As fluxes, separated by InAlAs.

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Control of Facets by Arsenic Flux

SiO2WCr

Increasing As flux

Original Interface

InAlAsmarkers

InGaAs

0.5x10-6

1x10-6

2x10-6

5x10-6

• Lowest arsenic flux → “rising tide fill”

• No gaps near gate or SiO2/SiNx

• Tunable facet competition

(Torr)

Growth conditions: MEE, 540*C, Ga+In BEP=1.5x10-7 Torr, InAlAs 500-540°C MBE.

• InGaAs:Si layers with increasing As fluxes, separated by InAlAs.

[111]

[100]

SiO

2

Filling[11

1]

[100]

SiO

2

[111]

[100]

SiO

2

Conformal

Faceting

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Low-As Regrowth of InGaAs and InAs

4.7 nm Al203, 5×1012 cm-2 pulse dopingIn=9.7E-8, Ga=5.1E-8 Torr

SEMs: Uttam Singisetti

InGaAs regrowth (top view)

• Low As flux good for InAs too.

• InAs native defects are donors. Bhargava et al , APL 1997

• Reduces surface depletion.

InAsregrowth

InGaAs InAs

• No faceting near gate• Smooth far-field too

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InAs Source-Drain Access Resistance4.7 nm Al203, InAs S/D E-FET.

• Upper limit: Rs,max = Rd,max = 370 Ω−μm.• Intrinsic gmi = 0.53 mS/μm• gm << 1/Rs ~ 3.3 mS/μm (source-limited case)

➡ Ohmic contacts no longer limit MOSFET performance.

740 Ω-µm

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Conclusions

• Reducing As flux improves filling near gate• Self-aligned regrowth: a roadmap for scalable III-V FETs

–Provides III-V’s with a salicide equivalent• InGaAs and relaxed InAs regrown contacts

–Not limited by source resistance @ 1 mA/µm–Results comparable to other III-V FETs... but now scalable

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Acknowledgements

• Rodwell & Gossard Groups (UCSB): Uttam Singisetti, Greg Burek, Ashish Baraskar, Vibhor Jain...

• McIntyre Group (Stanford): Eunji Kim, Byungha Shin, Paul McIntyre

• Stemmer Group (UCSB): Joël Cagnon, Susanne Stemmer

• Palmstrøm Group (UCSB): Erdem Arkun, Chris Palmstrøm

• SRC/GRC funding• UCSB Nanofab: Brian Thibeault, NSF