future prospects for moore’s law

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Future Prospects for Moore’s Law Eighth Annual High Performance Embedded Computing Workshop Lincoln Laboratory September 28, 2004 Robert Doering Texas Instruments, Inc.

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Future Prospects for Moore’s Law. Eighth Annual High Performance Embedded Computing Workshop Lincoln Laboratory September 28, 2004 Robert Doering Texas Instruments, Inc. Exponential trends in: More functions* per chip Increased performance Reduced energy per operation - PowerPoint PPT Presentation

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Page 1: Future Prospects for Moore’s Law

Future Prospects

for Moore’s Law

Future Prospects

for Moore’s Law

Eighth Annual High Performance

Embedded Computing Workshop

Lincoln Laboratory

September 28, 2004

Robert Doering

Texas Instruments, Inc.

Page 2: Future Prospects for Moore’s Law

Generalizations of Moore’s LawGeneralizations of Moore’s Law Exponential

trends in:

More functions* per chip

Increased performance

Reduced energy per operation

Decreased cost per function (the principal driver)

* transistors, bits, etc.

'69 '74 '79 '84 '89 '94 '99 '04

Source: DataQuest, Intel

10-2

10 -4

10-6

1

Price per Transistor in MPU ($)

Dollars to Microcents:

Page 3: Future Prospects for Moore’s Law

High-Level CMOS Technology Metrics– What are the Limits ?

High-Level CMOS Technology Metrics– What are the Limits ?

Component Diversity (integrated logic, memory, analog, RF, …)

Cost/Component (e.g., μ¢/gate or μ¢/bit in an IC)

Component Density (e.g., gates/cm2 or bits/cm2)

Logic Gate Delay (time for a gate to switch logic states)

Energy Efficiency (energy/switch and energy/time)

Mfg. Cycle Time (determines time-to-market for new designs as well as rate of yield learning)

All of these are limited by multiple factors inter-linked into a complex “tradeoff space.” We can only touch on a few of the issues today !

Page 4: Future Prospects for Moore’s Law

State-of-the-Art CMOS in 2004State-of-the-Art CMOS in 2004 ITRS Technology Node: 90 nm (half-pitch of DRAM metal lines)

4T-Gates/cm2: 37x106 (150 million transistors/cm2)

6T-eSRAM bits/cm2: 108 (600 million transistors/cm2)

Cost/Gate (4T): 40 μ¢ (high volume; chip area = 1 cm2)

Cost/eSRAM bit: 10 μ¢ (high volume; chip area = 1 cm2)

Gate Delay 24 ps * (for 2-input, F.O. = 3 NAND)

Switching Energy 0.5 fJ * (for inverter, half-cycle)

Passive Power 6 nW * (per minimum-size transistor)

Min. Mfg. Cycle Time 10 days (or 3 mask levels/day)

* Values at extreme tradeoff for MPU application

Page 5: Future Prospects for Moore’s Law

500

350

250

180

130

95 97 99 01 04 07 10 13 16

90

65

45

32

22

95 97 99 01 04 07 10 13 16

Scaling -- Traditional Enabler of Moore’s Law*Scaling -- Traditional Enabler of Moore’s Law*F

eat

ure

Siz

e [

nm

]

Year of Production

ITRS Gate Length

9

return to0.7x/3-yr ?

13

* For Speed, Low-Cost, Low-Power, etc.

ITRS Lithography Half-Pitch (DRAM)

Page 6: Future Prospects for Moore’s Law

Can We Extendthe Recent 0.7x/2-year Litho Scaling Trend ?

Can We Extendthe Recent 0.7x/2-year Litho Scaling Trend ?

30002000

15001000

400 350250

180 130

9065

45

500600

101

102

103

104

1980 1990 2000 2010

Year of Production

Abovewavelength

Nearwavelength

Belowwavelength

g-line=436nm

i-line=365nm

DUV=248nm 193

=193nm157

=157nm

32

=EUV 13.5nm

Ha

lf-P

itch

/ W

av

ele

ng

th (

nm

)

i-193‘=133nm

For lithography, it’s a question of cost and control/parametric-yield !

Page 7: Future Prospects for Moore’s Law

Com

plex

ity (m

ask,

use

)

Strength of enhancement

Illumination mode

Other (Tool)

Mask

Mask OPC

Resistk

1

0.25

0.5

A “Bag of Tricks” for Optical-ExtensionA “Bag of Tricks” for Optical-Extension

Conventional

Annular

Dipole

Soft Quasar

Custom

Scattering bars

Quasar

Binary Intensity Mask

Attenuated PSM 6%

Attenuated PSM 18%

Alternating PSM

Source: ASML

Serifs

Hammerheads

Line BiasingThick resist

Thin resist

Focus drilling

Phase filters

Double Exposures

Wavelength

NA

Of course : increasing complexity increasing cost !

Page 8: Future Prospects for Moore’s Law

Amortization of Mask Cost @ 130nmAmortization of Mask Cost @ 130nm

1

10

100

1000

1.00E+03 1.00E+04 1.00E+05 1.00E+06 1.00E+07 1.00E+08

Chips Produced

Co

st p

er C

hip

[$]

~ 1 million units required to get within 10% of asymptotic cost !(and getting worse with continued scaling)

Significant motivationfor some form of “mask-less lithography” !

Page 9: Future Prospects for Moore’s Law

Of course, overall scaling is limited

by more than just lithography !

Of course, overall scaling is limited

by more than just lithography ! Growing Significance of Non-Ideal Device-Scaling Effects:

ION vs. IOFF tradeoff

unfavorable and L scaling for interconnects

Approaching Limits of Materials Properties Heat removal and temperature tolerance

CMAX vs. leakage tradeoff for gate dielectric

CMIN vs. mechanical-integrity tradeoff for inter-metal dielectric

Increases in Manufacturing Complexity/Control Requirements cost and yield of increasingly complex process flows

metrology and control of LGATE, TOX, doping, etc.

Affordability of R&D Costs development of more complex and “near cliff” technologies

design of more complex circuits with “less ideal” elements

Page 10: Future Prospects for Moore’s Law

MP

U C

loc

k (G

Hz)

ITRS Tries to Address Top-Down GoalsITRS Tries to Address Top-Down Goals

2001

2003

Page 11: Future Prospects for Moore’s Law

Production Year: 2001 2004 2007 2010 2013 2016

Litho Half-Pitch [nm]: 130 90 65 45 32 22

Overlay Control [nm]: 45 32 23 18 13 9

Gate Length [nm]: 65 37 25 18 13 9

CD Control [nm]: 6.3 3.3* 2.2 1.6 1.2 0.8

TOX (equivalent) [nm]: 1.3-1.6 1.2 0.9 0.7 0.6 0.5

IGATE (LMIN) [µA/µm]: - 0.17 0.23 0.33 1 1.67

ION (NMOS) [µA/µm]: 900 1110 1510 1900 2050 2400

IOFF (NMOS) [µA/µm]: 0.01 0.05 0.07 0.1 0.3 0.5

Interconnect EFF- 3.1-3.6 2.7-3.0 2.3-2.6 2.0-2.4 <2.0

ITRS Highlights Scaling Barriers, e.g.:ITRS Highlights Scaling Barriers, e.g.:

Page 12: Future Prospects for Moore’s Law

Surface scattering becomes dominant

p=0 (diffuse scattering)p=1 (specular scattering)

0

1

2

3

4

5

0 100 200 300 400 500

Metal Line Width (nm)

Res

isti

vity

(μΩ

cm) p=0

p=0.5

Another Interconnect-Scaling IssueAnother Interconnect-Scaling Issue

Wire width < mean-free-path of electrons

Page 13: Future Prospects for Moore’s Law

2004 LG = 37-nm Transistor2004 LG = 37-nm Transistor

TOX(equiv.) = 1.2 nm

Page 14: Future Prospects for Moore’s Law

Can Some Hi-K Dielectric Replace SiON ? Can Some Hi-K Dielectric Replace SiON ?

Source: Intel

Sub-nm SiON:• mobility• uniformity• leakage

Page 15: Future Prospects for Moore’s Law

Selective-epi raised source/drainfor shallow junctions & reducedshort-channel effects

P-WELL

STI STISOURCE DRAIN

GATE

Si-Substrate

Halo I2

Etches for new materials that achieve profile, CD control, and selectivity

Metal gate electrode to reduce gate depletion

High- gate dielectric for reducing gate current with thin Tox

Strained channel forimproved mobility

Doping and annealing techniques for shallow abrupt junctions

Ni-silicide process for low resistanceat short gate lengths (near term)

In general, continued transistor scalingrequires new materials, processes, …

In general, continued transistor scalingrequires new materials, processes, …

Page 16: Future Prospects for Moore’s Law

Fin

BOx

Tri-Gate FET3 Gates

Fin

BOx/ Ω Gate FET

3+ Gates

Fin

BOx

FinFET2 Gates

ThickDielectric

ActiveGate

… and, eventually new structures… and, eventually new structures

Buried Oxide

Silicon

Si Si

Gate

Buried Oxide

Silicon

Steps toward ideal “coax gate”

Page 17: Future Prospects for Moore’s Law

Potential FET Enhancements ?Potential FET Enhancements ?

10

100

1000

500 1000 1500 2000 2500 3000Ion , µA/µm

Ioff

, nA

/µm

HP100

HP90

HP65

HP45

HP32

HP22 Bulk

+Strain

+UTB

SG

+Met.G

+UTB

DG

+Q. B

allis

tic+M

et. J

unc.

High PerformanceITRS 2003 Requirements

10

100

1000

500 1000 1500 2000 2500 3000Ion , µA/µm

Ioff

, nA

/µm

HP100

HP90

HP65

HP45

HP32

HP22 Bulk

+Strain

+UTB

SG

+Met.G

+UTB

DG

+Q. B

allis

tic+M

et. J

unc.

High PerformanceITRS 2003 RequirementsITRS 2003 Requirements

Calculations by T. Skotnicki

Page 18: Future Prospects for Moore’s Law

At PQE 2004, Professor Mark Lundstrom

expressed the outlook:

“Sub-10nm MOSFETs will operate, but …

At PQE 2004, Professor Mark Lundstrom

expressed the outlook:

“Sub-10nm MOSFETs will operate, but …

- on-currents will be ~0.5xIballistic, off-currents high,

- 2D electrostatics will be hard to control,

- parasitic resistance will degrade performance,

- device to device variations will be large,

and

- ultra-thin bodies and hyper-abrupt junctions will be essential”

Page 19: Future Prospects for Moore’s Law

Logic Device Technologies

Performance Architecture compatible

Stability and

reliability

CMOS compatible

Operate temp

Energy efficiency

Sensitivity parameter)

Scalability

1D Structures

2.3/2.2 2.2/2.9 1.9/1.2 2.3/2.4 2.9/2.9 2.6/2.1 2.6/2.1 2.3/1.6

RSFQ Devices

2.7/3.0 1.9/2.7 2.2/2.8 1.6/2.2 1.1/2.7 1.6/2.3 1.9/2.8 1.0/2.1

Resonant Tunneling Devices

2.6/2.0 2.1/2.2 2.0/1.4 2.3/2.2 2.2/2.4 2.4/2.1 1.4/1.4 2.0/2.0

Molecular Devices

1.7/1.3 1.8/1.4 1.6/1.4 2.0/1.6 2.3/2.4 2.6/1.3 2.0/1.4 2.6/1.3

Spin Transistor

2.2/1.7 1.7/1.6 1.7/1.7 1.9/1.4 1.6/2.0 2.3/2.1 1.4/1.7 2.0/1.4

SETs 1.1/1.2 1.7/1.2 1.3/1.1 2.1/1.4 1.2/1.8 2.6/2.0 1.0/1.0 2.1/1.7

QCA Devices 1.4/1.3 1.2/1.1 1.7/1.8 1.4/1.6 1.2/1.4 2.4/1.7 1.6/1.1 2.0/1.4

ITRS Assessment of Some Current Ideasfor Successors to CMOS Transistors

ITRS Assessment of Some Current Ideasfor Successors to CMOS Transistors

No obvious candidates yet for a CMOS replacement !

Page 20: Future Prospects for Moore’s Law

SRC Research Gap Analysis (for <50nm)SRC Research Gap Analysis (for <50nm)

Worldwide Funding ~ $1,386 M

WW Research Gap ~ $1,155M

Industry Funding(Semiconductors + Suppliers)

U.S. $313 M

Japan $142 M

Europe $ 74 M

~ $580 M

Asia-Pac $ 51 M

U.S. $329 M

Europe $249 M

Japan $125 M Government Funding

~ $806 M

Asia-Pacific $103 M

Ongoing Tasks $2,169M

New Tasks $372M

Worldwide Needs ~ $2,541 M

Page 21: Future Prospects for Moore’s Law

Extending Moore’s Law via Integrating New Functions onto CMOS

ITRS Emerging Technologies ?

“AnotherDimension”

Page 22: Future Prospects for Moore’s Law

Why “Moore’s Law” Is Still a Fun Topic !Why “Moore’s Law” Is Still a Fun Topic !

What makes us think that we can forecast more than

~5 years of future IC technology any better today ?!!

A 1975 IC Technology Roadmap