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Silicon Nano-Transistors and Breaking

the 10nm Physical Gate Length Barrier

Robert Chau, Brian Doyle, Mark Doczy,

Suman Datta, Scott Hareland, Ben Jin,

Jack Kavalieros and Matthew Metz

Components Research

Logic Technology Development

Intel Corporation

June 24 2003

(2)

2

Content

Introduction

Device Scaling trends and the 10nm L

G

barrier

New Device Structures

Gate Dielectric Scaling

(3)

3

Moore’s Law Continues…

Transistor # doubling every 2 years toward the 1 billion transistor microprocessor

1,000 10,000 100,000 1,000,000 10,000,000 100,000,000 1,000,000,000

1970 1980 1990 2000 2010

4004

8080 8086

8008

Pentium® Processor 486™ DX Processor

386™ Processor 286

Pentium® II Processor Pentium® III Processor

Pentium® 4 Processor

Heading toward 1 billion transistors in 2007

42 Million

(4)

4

Transistor Physical Gate Length Requirement

0.01 0.10 1.00

1990 1995 2000 2005 2010

Year

Mi

c

ro

n

Technology Node

Transistor Physical Gate

Length

0.5µm

0.35µm

0.25µm

0.18µm

0.13µm

90nm

65nm

45nm

30nm

130nm

70nm

50nm

30nm

20nm 15nm 0.2µm

(5)

5

Conventional Si Transistor Scaling

60nm

Lg = 30nm

LG= 10nm

65nm Node

45nm node

(6)

6

Content

• Introduction

Device Scaling trends and the 10nm L

G

barrier

• New Device Structures

• Gate Dielectric Scaling

(7)

7

Gate Delay and Energy-Delay Trends

1.E-02 1.E-01 1.E+00 1.E+01

0.001 0.01 0.1 1

LG (µm)

G a te D e la y (p s ) 10nm 20nm 15nm 1.E-05 1.E-04 1.E-03 1.E-02 1.E-01 1.E+00 1.E+01 1.E+02 1.E+03

0.001 0.01 0.1 1

LG (µm)

E n e rg y -D el ay P ro d u c t (x 10 -2 7 j o ul es .s ec ) 20nm 10nm 15nm

(8)

8

Experimental 15nm Si Nano-Transistor

0 100 200 300 400 500

0 0.2 0.4 0.6 0.8

Drain Voltage (V)

Drain Current (µ A /µ m )

Vg = 0.8V

0.7V 0.6V 0.5V 0.4V 0.3V 15nm NMOS 1.E-08 1.E-07 1.E-06 1.E-05 1.E-04 1.E-03

0 0.2 0.4 0.6 0.8

Gate Voltage (V)

Drain Current (A/

µ

m)

Vd = 0.8V

Vd = 0.05V

S.S. = 95mV/decade DIBL = 100mV/V Ioff = 180nA/um 15nm NMOS

Electrostatics of 15nm transistor remains intact

(9)

9

Experimental 10nm MOS Transistor

LG = 10nm 0

200 400 600

0 0.2 0.4 0.6 0.8

Drain Voltage (V)

Drain Current (A/

µ

m)

0

0 0.2 0.4 0.6 0.8 0 0.2 0.4 0.60.6 0.8

0.75V 0.65V 0.55V 0.45V 1.E-08 1.E-07 1.E-06 1.E-05 1.E-04 1.E-03

-0.3 0.0 0.3 0.6 0.9 Gate Voltage (V)

Id ( A /¬ m) `

10nm transistor shows degraded short channel performance

high Ioff

0.75V

(10)

10

Transistor Off-state Leakage Trend

1.E-14 1.E-12 1.E-10 1.E-08 1.E-06 1.E-04

10 100 1000

Lg (nm)

Ioff

(A/um)

Intel 10nm device

Intel 15nm device Production Data

(11)

11

Leakage Power is becoming a

Larger % of Total Chip Power

-Total Power (Watts)

10

100

1,000

0.25u 0.18u 0.13u 90nm 65nm 45nm

Off-State Leakage Active Power

2V 1.7V 1.5V 1.2V 1V 0.9V

Total Power (Watts)

10

100

1,000

0.25u 0.18u 0.13u 90nm 65nm 45nm

Off-State Leakage Power Active Power

2V 1.7V 1.5V 1.2V 1V 0.9V

(12)

12

Potential Solutions to Transistor

I

off

Problem

Low-temperature operation

Improve short-channel performance

(subthreshold slope & DIBL) using

novel device structures

Fully-Depleted Transistors

Single-gate planar fully depleted SOI

Double-gate FINFET

(13)

13

Content

• Introduction

• Device Scaling trends and the 10nm L

G

barrier

New Device Structures

• Gate Dielectric Scaling

(14)

14

Si TSi

Lg

Si T

Planar fully depleted SOI

Fully Depleted Transistors

Double-gate (e.g. FINFET)

W

Si

L

g

TSi

Isolation

(Non-Planar)

(Planar)

W

Si

L

g

T

Si

Tri-gate

(Non-Planar)

(15)

15

Planar Fully Depleted Transistors

Si TSi

L

g

Si

SiO2

T

1E-09 1E-08 1E-07 1E-06 1E-05 1E-04 1E-03

0 0.25 0.5 0.75 1 1.25

VG (Volts)

ID

(A/

µ

m)

DST

Bulk Silicon

VD = 1.3V

VD = 0.05V

FD-SOI

Planar Fully Depleted SOI

Fully depleted SOI provides steeper subthreshold slope

and better DIBL, which can be used to reduce Ioff or increase Idsat

(16)

16

Planar Fully-depleted SOI

Lg = 60nm

Epi Raised S-D

T

Si

~18 nm

Silicide

BOX

Raised S-D using Selective Epi-Si Deposition

(17)

17

Tri-gate Transistor

WSi

L

g

Top Gate

Side Gate Side Gate

T

Si S/D

D/S

Gate

Top Gate

Side Gate

Side Gate

(18)

18

Si TSi

Lg Si T WSi

L

g TSi WSi Lg TSi

0 20 40 60 80

Device Gate Length, Lg (nm)

Silicon Body Thickness

(nm

)

Single-Gate

Double-Tri-Gate

0 20 40 60 80

Single- Gate

Tri-Gate

0 20 40 60 80

-0 10 20 30 40 50

0 20 40 60 80

Double-Gate

-60

(TSi) (WSi) (TSi, WSi)

3X

1.5X

(19)

19

VG(Volts)

1E 09 1E-08 1E-07 1E-06 1E-05 1E-04 1E-03

-1.4 -1 -0.6 0.6 1 1.4

I d

(|A/

µ

m|)

Vd=-0.05V Vd= 0.05V

Vd=1.3V

-0.2 0.2

nMOS pMOS

Vd=-1.3V

Non-Planar Tri-Gate CMOS Transistor

Silicon Body Buried Oxide 36 nm 55 nm Poly

Lg = 60nm

Silicon Body Buried Oxide 36 nm 55 nm Poly

Lg = 60nm

LG = 60nm

Lg = 60nm

TSi= 36 nm

WSi= 55 nm

Current per unit width = Id/(2*TSi+WSi)

DIBL < 50mV/V, S.S. ~ 69mV/decade

(20)

20

Tri-Gate Device Physics

Three distinct regions of operation

Oxide

Top channel

(21)

21

Components of Current in Tri-Gate

Vg (V)

Id (A/

µ

m)

1.0E-09

01.0E-8

1.0E-07

1.0E-06

1.0E-05

1.0E-04

1.0E-03

1.0E-02

0.0

0.2

0.4

0.6

0.8

1.0

Non-Corner

Total

Corner

Vd=1.0V

Vd=0.05V

(22)

22

Physics of Corner Device

Vg=0.5V, Vd=1.0V Cut at midpoint along channel

Proximity of the two gates at the corner give the

(23)

23

Tri-Gate Architecture

Gate Si Legs

Gate

Silicon Legs

S D

G

Multiple

Legs

Total Drive Current =

Id per Tri-gate Transistor x no. of Legs

S D

G

Source

Drain Gate

(24)

24

Nano-Device Structure Evolution

Gate

Nanowire

Non-Planar Tri-gate

Gate

GateGate

Silicon Substrate

SiO2

SiO2

Gate

Silicon Substrate

SiO2

SiO2

Planar Transistor

S D

G

Gate

(25)

25

Content

• Introduction

• Device Scaling trends and the 10nm L

G

barrier

• New Device Structures

Gate Dielectric Scaling

(26)

26

SiO2 Less Than 3 Atomic layers Thick

PolySi

Silicon PolySi

Silicon

SiO2

SiO2 leakage is increasing with reducing thickness

SiO2 gate oxide running out of atoms for further scaling 0.0

0.5 1.0 1.5 2.0

-1 -0.5 0 0.5 1

Vg C a pacita nce ( µ F/cm²) NMOS PMOS NMOS PMOS --0.0 0.5 1.0 1.5 2.0

-1 -0.5 0 0.5 1

(27)

27

Alternative Gate Dielectric Required for

Future-Generation Si Nano-Transistors

1.E-06 1.E-04 1.E-02 1.E+00 1.E+02 1.E+04

5 10 15 20 25

EOT [A]

J

ox

[A/cm

2 ]

SiO2 Dielectric

High-K

Dielectric

(28)

28 ƒ

NMOS: Ft = 83GHz Fmax = 35GHz

ƒ

PMOS: Ft = 41GHz Fmax = 25GHz

Si CMOS Transistor with Alternative

Gate Dielectrics

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0

-1.5 -1 -0.5 0 0.5 1 1.5

Vds (V)

Ids

(mA/

µ

m)

Vgs-Vth= 1.25V

Vgs-Vth= 0.75V

Vgs-Vth= 0.25V Vgs-Vth= -1.25V

Vgs-Vth= -0.75V

Vgs-Vth= -0.25V

PMOS NMOS 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0

-1.5 -1 -0.5 0 0.5 1 1.5

Vds (V)

Ids

(mA/

µ

m)

Vgs-Vth= 1.25V

Vgs-Vth= 0.75V

Vgs-Vth= 0.25V Vgs-Vth= -1.25V

Vgs-Vth= -0.75V

Vgs-Vth= -0.25V

PMOS NMOS

(29)

29

Summary

Research Si nano-transistors down to 10nm physical LG

have been demonstrated with improved intrinsic gate delay and energy-delay trends over devices with longer LG

Transistor off-state leakage increases with reducing

physical LG, and will need to be reduced for future logic products

10nm research transistor exhibits degraded short channel performance and high off-state leakage

Gate oxide leakage is increasing with reducing thickness and SiO2 is running out of atoms for further scaling

Referensi

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