FinFET 3D Transistor & the Concept Behind It Chenming Hu Univ. - - PowerPoint PPT Presentation

finfet 3d transistor the concept behind it
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FinFET 3D Transistor & the Concept Behind It Chenming Hu Univ. - - PowerPoint PPT Presentation

FinFET 3D Transistor & the Concept Behind It Chenming Hu Univ. of Calif. Berkeley http://www.eecs.berkeley.edu/~hu/ 1 Chenming Hu, August 2011 May 4 2011 NY Times Front Page Intel will use 3D FinFET at 22nm Most radical change in


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SLIDE 1

FinFET 3D Transistor & the Concept Behind It

Chenming Hu, August 2011 1

Chenming Hu

  • Univ. of Calif. Berkeley

http://www.eecs.berkeley.edu/~hu/

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SLIDE 2

2

  • Intel will use 3D FinFET at 22nm
  • Most radical change in decades
  • There is a competing SOI

technology

May 4 2011 NY Times Front Page

Chenming Hu, August 2011 2

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New MOSFET Structures

Chenming Hu, August 2011

Cylindrical FET Ultra Thin Body SOI

3

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  • Vt, S, Ioff are bad &

sensitive to Lg

  • Dopant fluctuations.

Requiring

  • higher Vt, Vdd, and

power consumption

  • higher design cost

Good Old MOSFET Nearing Limits

Finally painful enough for change.

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0.0 0.3 0.6 0.9 10

  • 11

10

  • 9

10

  • 7

10

  • 5

10

  • 3

Drain Current, IDS (A/µm) Gate Voltage, VGS (V)

Size shrink

Smaller size

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SLIDE 5

Why Vt Variation & Swing are So Bad

L Gate Oxide Source Drain

Cg Cd

Gate

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0.0 0.3 0.6 0.9 10

  • 11

10

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  • 5

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  • 3

Drain Current, IDS (A/µm) Gate Voltage, VGS (V) Size shrink

Smaller size

MOSFET becomes “resistor” at very small L – Drain competes with Gate to control the channel barrier.

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SLIDE 6

Making Oxide Thin is Not Enough Gate cannot control the leakage current paths that are far from the gate.

Gate Source Drain

Leakage Path

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C.Hu,”Modern Semicon. Devices for ICs” 2010, Pearson

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SLIDE 7

One Way to Eliminate Si far from Gate

Gate Gate Source Drain

FinFET body is a thin fin

  • N. Lindert et al., DRC paper II.A.6, 2001

Source Drain

Fin Width Fin Height Gate Length

Chenming Hu, August 2011 7

A thin body controlled by gate from more than one side.

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SLIDE 8

FinFET- 1999

Undoped Body. 30nm etched thin fin. Vt set with gate work-function.

  • X. Huang et al., IEDM, p. 67, 1999
  • 0.6
  • 0.4
  • 0.2

0.0 0.2 0.4 0.6 10 20 30 40 50

Lg [nm] ΔVt [V]

Vt at 100 nA/μm, Vd = 0.05 V

Fin width: 20 nm

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SLIDE 9

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FinFET is “Easy” to Scale

Leakage is well suppressed if Fin thickness =or< Lg

  • Thin fin and gate can be made with the

same lithography and etching tools.

Chenming Hu, August 2011

Lg = 5 nm

5nm Lg TSMC 2004 VLSI Symp 10nm Lg AMD 2002 IEDM 3nm Lg KAIST 2006 VLSI Symp

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SLIDE 11

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FinFET Leakage Path

S D

C.Hu,”Modern Semicon. Devices for ICs” 2010, Pearson

Body thickness is the new scaling parameter.

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SLIDE 12

Two Improvements to FinFET

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Original FinFET had thick oxide on fin top & used SOI for process simplicity.

  • 2002 FinFET with thin oxide on fin top.

F.L.Yang et al. (TSMC) 2002 IEDM, p. 225.

  • 2003 FinFET on bulk substrate.
  • T. Park et al. (Samsung) 2003 VLSI Symp.
  • p. 135.
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SLIDE 13

STI Gate Si STI STI Gate Si STI

State-of-the-Art FinFET

20nm Hi Perf C.C. Wu et al., 2010 IEDM

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2nd Way to Eliminate Si far from Gate

Ultra-thin-body SOI (UTB-SOI)  No leakage path far from the gate.

1.E-12 1.E-10 1.E-08 1.E-06 1.E-04 1.E-02 0.2 0.4 0.6 0.8 1

Gate Voltage [V] Drain Current [A/um] Tsi=8nm Tsi=6nm Tsi=4nm

Y-K. Choi, IEEE EDL, p. 254, 2000

Gate Source Drain UTB

SiO2 Si

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SLIDE 15

Most Leakage Flows >5nm Below Surface

Y-K. Choi et al., IEEE Electron Device Letters, p. 254, 2000

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SLIDE 16

Silicon Body Needs to be <Lg/3

For good swing and device variation

Y-K. Choi et al., IEEE Electron Device Letters, p. 254, 2000

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SLIDE 17

Y-K. Choi et al, VLSI Tech. Symposium, p. 19, 2001

3nm Silicon Body, Raised S/D

UTB-SOI

Chenming Hu, August 2011 17

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SLIDE 18

State-of-the-Art 5nm Thin-Body SOI

ETSOI, IBM

  • K. Cheng et al, IEDM, 2009

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SLIDE 19

Both Thin-Body Transistors Provide

  • Better swing.
  • S & Vt less sensitive to Lg and Vd.
  • No random dopant fluctuation.
  • No impurity scattering.
  • Less surface scattering (lower Eeff).
  • Higher on-current and lower leakage
  • Lower Vdd and power consumption
  • Further scaling and lower cost

Chenming Hu, August 2011 19

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SLIDE 20

Similarities between FinFET & UTBSOI Device Physics

  • Superior S, scalability and device variations
  • use body thickness as a new scaling parameter
  • can use undoped body for high µ and no RDF

History

  • 1996: UC Berkeley proposed both to DARPA

as “25nm Transistors”.

  • 1999: demonstrated FinFET

2000: demonstrated UTB-SOI

  • Since 2001: ITRS highlights FinFET and UTBSOI

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Main Differences

  • FinFET body thickness ~Lg. Investment by fab.

UTBSOI thickness ~1/3 Lg. Investment by Soitec.

  • FinFET has clearer long term scalability.

UTBSOI may be ready sooner than FinFET for some companies.

  • FinFET has larger Ion.

UTBSOI has a good back-gate bias option.

STI STI Si Gate 1 Gate 2

UTBSOI FinFET

Chenming Hu, August 2011 21

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What May Happen

  • FinFET will be used at 22nm by Intel and

later by more firms to <10nm.

  • Some firms may use UTBSOI to gain market

from regular CMOS at 20/18/16nm. If so, competition between FinFET and UTBSOI will bring out the best of both.

Chenming Hu, August 2011 22

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Berkeley Short-channel IGFET Model

  • 1997: became first industry standard

MOSFET model for IC simulation

  • BSIM3, BSIM4, BSIM-SOI used by

hundreds of companies for design of ICs worth half trillion dollars

  • BSIM models of FinFET and UTBSOI

are available – free 

BSIM SPICE Models

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  • FinFET and UTB-SOI allows lower Vt

and Vdd  Lower power.

  • Body thickness is a new scaling

parameter  Better short channel effects to and beyond 10nm.

  • Undoped body  Better mobility and

random dopant fluctuation.

  • BSIM models of FinFET and UTBSOI

are available – free 

Summary

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