The Red Brick Wall of Traditional Semiconductor Electronics The ...
The Red Brick Wall of Traditional Semiconductor Electronics The ...
The Red Brick Wall of Traditional Semiconductor Electronics The ...
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<strong>The</strong> <strong>Red</strong> <strong>Brick</strong> <strong>Wall</strong> <strong>of</strong> <strong>Traditional</strong><br />
<strong>Semiconductor</strong> <strong>Electronics</strong><br />
H. Jörg Osten<br />
Institute for <strong>Semiconductor</strong> Devices<br />
and Electronic Materials<br />
University <strong>of</strong> Hannover
150 Years <strong>of</strong> <strong>Electronics</strong><br />
Edison Effect<br />
Lilienfeld<br />
Patents<br />
Diode &Triode<br />
Vacuum Tubes<br />
Point Contact<br />
& Junction Transistors<br />
I.C. MOS Silicon Gate<br />
Scaling, Scaling<br />
<strong>Traditional</strong> Equivalent<br />
’70 ’80 ’90 ’00 ’10 ’20 ’30 ’40 ’50 ’60 ’70 ’80 ’90 ’00 ’10 ’20<br />
19th Century 20th Century 21st Century
“I think there is a world market for<br />
maybe five computers”<br />
Thomas Watson Senior,<br />
Chairman <strong>of</strong> IBM, 1943
<strong>The</strong> Birth <strong>of</strong> Microelectronics<br />
23.12. 1947:<br />
<strong>The</strong> first Ge point contact device<br />
showed a current gain <strong>of</strong> 18<br />
(Bell Laboratories)<br />
Current Transfer + Resistor = Transistor
Silicon Wafer Today
<strong>The</strong> Intel Family<br />
10 M<br />
1M<br />
A new processor every 2-3 years !<br />
Transistors<br />
100K<br />
10K<br />
4004<br />
1975 1980 1985 1990 1995 2000<br />
Pentium III<br />
8080<br />
8086<br />
80286<br />
80486<br />
80386<br />
Pentium<br />
Pentium II
<strong>Electronics</strong>, Vol. 38, Nr. 8, April 19, 1965
Moore’s “Law”<br />
<strong>The</strong> number <strong>of</strong> transistors per chip<br />
doubles every 18 months
CPU MHz Trend<br />
MHz<br />
1000<br />
100<br />
10<br />
8080<br />
8086<br />
286<br />
Pentium(R)Pro Processor<br />
Pentium(R) Processor<br />
386TM<br />
486TM<br />
1<br />
1970 1980 1990 2000 2010<br />
YEAR<br />
1.25x per year
DRAM Cost Per Function<br />
100000<br />
Price per bit (Millicents)<br />
10000<br />
1000<br />
100<br />
10<br />
1<br />
0,1<br />
'65 '70 '75 '80 '85 '90 '95 2000
<strong>Semiconductor</strong> End Markets 2003<br />
12%<br />
12%<br />
11%<br />
10% 8%<br />
30%<br />
17%<br />
PC<br />
other Computer<br />
Cell phones<br />
other Commun.<br />
Industrial/Military<br />
Automotive<br />
Consumer<br />
Source: SIA 2003
What is the „ „Best „Best“ est“ “ Technology<br />
Technology?<br />
echnology?<br />
Simplicity<br />
Simplicity<br />
Reliability<br />
Reliability<br />
Needed Needed tools tools<br />
&<br />
investments<br />
Production cost<br />
Production cost<br />
Integration Integration in in<br />
existing existing processes processes<br />
CMOS<br />
III/V III/V-Devices<br />
Devices<br />
Si Si-Bipolar<br />
Bipolar<br />
Si Si-BiCMOS<br />
BiCMOS<br />
SiGe SiGe-Bipolar<br />
Bipolar<br />
SiGe SiGe-BiCMOS<br />
BiCMOS<br />
......... .........<br />
Needed Needed device device<br />
parameter parameter<br />
Power consumption<br />
Power consumption<br />
Maturity<br />
Maturity<br />
Environmental<br />
issues issues
What is the „ „Best“<br />
est“ Technology?<br />
echnology?<br />
<strong>The</strong> “best technology“ depends on<br />
desired application<br />
As cheap as possible<br />
As established as possible<br />
Performance only sufficiently high
Major Technologies 2003<br />
Global market: $154.9 B<br />
Billion $<br />
13.3<br />
8.3<br />
25.8<br />
25.8<br />
10.3<br />
6.2<br />
34.3<br />
15.7<br />
9.7<br />
5.5<br />
Products<br />
Discrete<br />
Optoelectronics<br />
Analog<br />
MOS µ-processors<br />
MOS µ-controllers<br />
MOS DSP<br />
MOS Logic<br />
MOS DRAM<br />
Flash EEPROMS<br />
others<br />
4%<br />
6.6%<br />
17%<br />
more than 90 % is based on Si<br />
more than 80 % is integrated<br />
17%<br />
22%<br />
10%<br />
5.4% 8.6%<br />
6.3%<br />
3.6%<br />
Source: SIA 2003
It is revolutionary time ...<br />
Processor: 30% more components per year,<br />
doubling in speed every 1.5 years<br />
Memory: 60% more capacity every year<br />
Harddisk: 60% more capacity every year<br />
Cost per function: 25% lower every year
Moore‘s Law Law:<br />
: New Structures<br />
1960‘s: Bipolar, Mesa, Metal gate<br />
1970‘s: MOS, Poly-gate, LOCOS isolation<br />
1980‘s: CMOS, W plugs, salicide process<br />
1990‘s: STI isolation, BiCMOS, CMP,<br />
multilevel metal, SiGe bipolar<br />
2000‘s: Hetero MOS (strained silicon), …
Moore‘s Law Law:<br />
: New Materials<br />
1960‘s: Si, Al, SiO 2<br />
1970‘s: Poly-Si, PSG, Al-Si, Si 3 N 4<br />
1980‘s: BPSG, WSi 2 , Polyimide, SOG, TiN, TiN<br />
1990‘s: Al-Cu, W, MoSi 2 , SiOF, Cu, SiGe,<br />
TiSi 2 , CoSi 2 , Low-K ILD<br />
2000‘s: High-K dielectrics, …?
CMOS Technology Breakthrough Takes Time…<br />
Tool or Technology<br />
Silicon epitaxy<br />
APCVD silicon nitride<br />
Ion implantation<br />
TiW metallization<br />
Charge-coupled devices (CCD)<br />
Reactive ion etch (RIE)<br />
Poly-Si emitter<br />
Refractory gate<br />
SIMOX (SOI via implantation)<br />
Trench capacitors<br />
Silicide (self-aligned)<br />
Lightly-doped drain (LDD)<br />
developed<br />
1960<br />
1965<br />
1969<br />
1970<br />
1970<br />
1975<br />
1976<br />
1976<br />
1978<br />
1979<br />
1978<br />
1980<br />
In production<br />
1964<br />
1968<br />
1973<br />
1976<br />
1981<br />
1980<br />
1984<br />
1983<br />
1989<br />
1986<br />
1985<br />
1986<br />
∆<br />
4<br />
4<br />
4<br />
6<br />
11<br />
5<br />
8<br />
7<br />
11<br />
7<br />
7<br />
6
Moore’s Law today today:<br />
: New Capabilities<br />
Resist, optics, mask (157nm, EUV, …)<br />
Chemical-mechanical polishing<br />
Deposition <strong>of</strong> high-K dielectrics<br />
Low-K dielectrics (organics) integration<br />
Thinner conformal barrier metals<br />
Higher thermal conductivity materials<br />
Atomic layer conformal deposition
Example: Hetero Heterojunction<br />
junction Bipolar<br />
ipolar Transistor (HBT)<br />
Poly SiGe:C/Si<br />
STI<br />
W<br />
SiGe:C<br />
W<br />
Emitter<br />
window<br />
Active region<br />
As doped<br />
emitter<br />
XTEM image <strong>of</strong> a SiGe:C HBTs<br />
Thin, heteroepitaxial<br />
base layer<br />
IHP 2001
HBT: Bor Boron<br />
on Outdiffusion – the Key Problem<br />
n-emitter (Si) p-base (SiGe) n-collector (Si)<br />
Boron doping
HBT: Bor Boron<br />
on Outdiffusion – the Key Problem<br />
n-emitter (Si) p-base (SiGe) n-collector (Si)<br />
Boron doping
Boron Outdiffusion: <strong>The</strong> Problem<br />
Conduction band for heavily p-doped Si and SiGe (schematically)<br />
npn-Si<br />
npn-Si/SiGe/Si<br />
Parasitic barriers
Material Solution:<br />
Suppression <strong>of</strong> Boron Outdiffusion by Carbon<br />
SiGe<br />
B concentration<br />
BORON<br />
Annealing<br />
Depth (nm) Depth (nm)<br />
SIMS investigations on real devices<br />
SiGe:C<br />
B concentration
SUMMARY: Dopant Diffusion in Si SiGe SiGe:C Ge:C :C<br />
Model <strong>of</strong> C outdiffusion provides quantitative<br />
description<br />
– Coupled diffusion <strong>of</strong> C and Si point defects<br />
Suppressed B diffusion due to C incorporation<br />
– Interstitial undersaturation due to C outdiffusion<br />
– diffusivity reduction <strong>of</strong> ~20 for < 10 20 cm -3 C<br />
C suppresses also transient enhanced diffusion (TED)<br />
during damage annealing<br />
Boron and phosphorous diffusion is suppressed by C<br />
– Interstitial-mediated dopant diffusion<br />
Antimony and arsenic diffusion is enhanced by C<br />
– Vacancy-mediated dopant diffusion
SiGe:C Heterojunction Bipolar Transistor<br />
f T or f max (GHz)<br />
75<br />
70<br />
65<br />
60<br />
55<br />
50<br />
45<br />
40<br />
35<br />
30<br />
- First realization with MBE 1997 -<br />
10 -3<br />
f max<br />
V CE = 2 V<br />
Emitter Area 0.5 x 5 µm²<br />
R SBi = 2.3 kΩ<br />
f T<br />
Collector Current (A)<br />
10 -2<br />
Ring Oscillator Delay<br />
CML-type, FI/FO = 1<br />
25 HBTs, 0.9 x1.3 µm²<br />
td ± σ =<br />
(12.9 ± 0.2) ps<br />
best value: 12.6 ps<br />
Osten et al. IEDM 97<br />
Meanwhile both frequencies are above 200 GHz<br />
Si-based analog circuits for mobile communication
Modular Integration: BiCMOS ffor<br />
for or Everybody<br />
“bipolar step<br />
proce ss step<br />
“corrected”<br />
CMOS<br />
CMOS<br />
classical<br />
BiCMOS<br />
bipolar<br />
modul<br />
modular<br />
odular<br />
BiCMOS
Modular Integration <strong>of</strong> SiGe:C HBTs in into<br />
to CMOS<br />
CMOS<br />
digital<br />
+<br />
HBT<br />
=<br />
BiCMOS<br />
• IHP module can be integrated into nearly any CMOS process<br />
• No changes in CMOS flow (modular integration)<br />
• CMOS libraries can be re-used<br />
• Adds only 4 additional masks to the process<br />
• Requires only epi-SiGe:C CVD as a new step
Prognosis ….<br />
“<strong>The</strong>re is no reason anyone<br />
would want a computer in<br />
their home”<br />
Ken Olsen<br />
President, Chairman and<br />
founder <strong>of</strong> Digital, 1977
<strong>The</strong> Coming Years<br />
Consult the<br />
oracle<br />
ITRS Roadmap
<strong>The</strong> ITRS Consortium<br />
onsortium<br />
TWG Members by Regions TWG Members by Affiliations<br />
Japan<br />
222<br />
26%<br />
19%<br />
Taiwan<br />
161<br />
Korea<br />
64<br />
8%<br />
USA<br />
324<br />
39%<br />
8%<br />
Europe<br />
68<br />
Source: 2001 ITRS - Exec. Summary<br />
Research Inst. /<br />
Consortia / Other<br />
University 1% 10<br />
193 23%<br />
22%<br />
Equipment /<br />
Materials<br />
Suppliers 185<br />
Chip Makers<br />
445<br />
54%
<strong>The</strong> Plan for Globalization - ITRS Working Groups<br />
International<br />
Technology<br />
Working Groups<br />
(ITWG)<br />
Design<br />
Test<br />
Front End Processes<br />
Interconnect<br />
Lithography<br />
Process Integration<br />
Assembly & Packaging<br />
Factory Integration<br />
International Crosscut Technology<br />
Working Group (ICCT WG)<br />
Environment<br />
Safety &<br />
Health<br />
Metrology Defect<br />
<strong>Red</strong>uction<br />
Modeling &<br />
Simulation<br />
http://public.itrs.net
<strong>The</strong> latest ITRS Roadmap ( (selected selected example example)<br />
Year <strong>of</strong> Production:<br />
DRAM Half-Pitch [nm]:<br />
Overlay Accuracy [nm]:<br />
MPU Gate Length [nm]:<br />
CD Control [nm]:<br />
T OX (equivalent) [nm]:<br />
Junction Depth [nm]:<br />
Metal Cladding [nm]:<br />
Inter-Metal Dielectric K:<br />
2001<br />
130<br />
46<br />
90<br />
8<br />
1.3-1.6<br />
48-95<br />
16<br />
3.0-3.6<br />
2003<br />
100<br />
35<br />
65<br />
5.5<br />
1.1-1.8<br />
33-66<br />
12<br />
3.0-3.6<br />
2005<br />
80<br />
28<br />
45<br />
3.9<br />
0.8-1.3<br />
24-47<br />
9<br />
2.6-3.1<br />
2007<br />
65<br />
23<br />
35<br />
3.1<br />
0.6-1.1<br />
18-37<br />
7<br />
2.3-2.7<br />
2010<br />
45<br />
18<br />
25<br />
2.2<br />
0.5-0.8<br />
13-26<br />
5<br />
2.1<br />
2016<br />
22<br />
9<br />
13<br />
1.1<br />
0.4-0.5<br />
7-13<br />
Solution known R&D needed Solution unknown<br />
2.5<br />
1.8
<strong>The</strong> <strong>Red</strong> <strong>Brick</strong> <strong>Wall</strong> <strong>of</strong> Microelectronics<br />
Year <strong>of</strong> Production:<br />
DRAM Half-Pitch [nm]:<br />
Overlay Accuracy [nm]:<br />
MPU Gate Length [nm]:<br />
CD Control [nm]:<br />
T OX (equivalent) [nm]:<br />
Junction Depth [nm]:<br />
Metal Cladding [nm]:<br />
Inter-Metal Dielectric K:<br />
2001<br />
130<br />
46<br />
90<br />
8<br />
1.3-1.6<br />
48-95<br />
16<br />
3.0-3.6<br />
2003<br />
100<br />
35<br />
65<br />
5.5<br />
1.1-1.8<br />
33-66<br />
12<br />
3.0-3.6<br />
2005<br />
2.6-3.1<br />
2007<br />
0.6-1.1<br />
18-37<br />
2.3-2.7<br />
Solution known R&D needed Solution unknown<br />
80<br />
28<br />
45<br />
3.9<br />
0.8-1.3<br />
24-47<br />
9<br />
65<br />
23<br />
35<br />
3.1<br />
7<br />
2010<br />
45<br />
18<br />
25<br />
2.2<br />
0.5-0.8<br />
13-26<br />
5<br />
2.1<br />
2016<br />
22<br />
9<br />
13<br />
1.1<br />
0.4-0.5<br />
7-13<br />
2.5<br />
1.8
Ultrathin Gate oxide oxide: : 30 nm Transistor<br />
30 nm FET (Intel)
Need for Alternative Gate Dielectrics<br />
Production<br />
year<br />
Technology<br />
Node<br />
(nm)<br />
Gate dielectric<br />
(SiO2 equivalent)<br />
thickness<br />
(Å)<br />
Gate bias, Vdd<br />
(V)<br />
Leakage current<br />
for SiO2 @ Vdd<br />
(for max. EOT)<br />
(A/cm²)<br />
2001 130 13 - 16 1.1 > 0.1<br />
2002 115 12 - 16 1.0 > 0.1<br />
2003 100 11 - 16 1.0 > 0.1<br />
2004 90 9 - 14 1.0 > 1<br />
2005 80 8 - 13 0.9 > 2<br />
2006 70 7 - 12 0.9 > 5<br />
2007 65 6 -11 0.7 > 10<br />
2010 45 5 - 8 0.6 > 100<br />
2013 32 4 - 6 0.5<br />
2016 22 4 - 5 0.4
Alternatives<br />
Needed: thicker gate dielectric<br />
BUT: <strong>The</strong> capacity cannot be changed!<br />
C ~ K A / t<br />
Solution: Materials with higher dielectric constant (High-K)<br />
For a given capacitance, the possible layer thickne ss scale s with K<br />
Capacitance scales linearly with thickness<br />
Equivalent Oxide Thickne ss: EOT = t * 3.9/K
“High “High-K”<br />
K” Diele Dielectri Dielectrics: trics cs: Requirements<br />
Dielectric constant between 15 and 40<br />
Chemical Stability against silicon<br />
– No tendency for silicide formation<br />
– No tendency for silicon o xide interfacial layer formation<br />
Compatibility with CMOS Process<br />
– Includes thermal stability<br />
– Selective etching<br />
Important parameter:<br />
– Interface trap density (D it ) impacts carrier mobility<br />
– Sufficiently high K and suitable band <strong>of</strong>fsets to Si impacts<br />
leakage current (for FET and memory)<br />
Epitaxia l?
Search for Suitable Binary Oxides<br />
H not solid at 1000K He<br />
Li Be radioactive B C N O F Ne<br />
Na Mg Al Si P S Cl Ar<br />
K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr<br />
Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe<br />
Cs Ba * Lu Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn<br />
Fr Ra ** Lr Rf Db Sg Bh Hs Mt<br />
* Lanthanoids La Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb<br />
** Actinoids Ac Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No
Search for Suitable Binary Oxides<br />
Si + MOx M+SiO2 ; MSiz + SiO2 ; M + MSixOy<br />
H not solid at 1000K He<br />
Li Be radioactive B C N O F Ne<br />
Na Mg Also not suitable Al Si P S Cl Ar<br />
K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr<br />
Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe<br />
Cs Ba * Lu Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn<br />
Fr Ra ** Lr Rf Db Sg Bh Hs Mt<br />
* Lanthanoids La Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb<br />
** Actinoids Ac Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No
Praseodym<br />
Praseodymium<br />
ium Oxid Oxide: xide: : Leakage Current<br />
J g (A/cm -2 )<br />
10 2<br />
10 0<br />
10 -2<br />
10 -4<br />
10 -6<br />
10 -8<br />
10 -10<br />
10 -12<br />
16 Au/Pr 2O 3/n-Si capacitors<br />
1.9 x 10 -3 cm², EOT = 1.4 nm.<br />
-2 0 2 4 6 8<br />
V g (V)<br />
Leakage current density for different<br />
dielectrics with EOT = 1.4 nm.<br />
Material Jg (A/cm ²)<br />
@ Vg = 1V<br />
Pr2O3<br />
HfO2<br />
ZrO2<br />
SiO2<br />
7*10 -9<br />
1*10 -4<br />
5*10 -4<br />
~ 1<br />
SiO2 (3 nm ) ~ 10 -4<br />
Osten et al. IEDM 2000<br />
Lowest reported values for leakage current
Pr 2O 2O3 Growth 3 Growth on Si(111)<br />
5 nm<br />
epi Si<br />
h-Pr 2 O 3<br />
(111) Si<br />
X-HREM <strong>of</strong> a 6 nm<br />
thick, hexagonal Pr 2 O 3<br />
film grown epitaxially<br />
on a Si(111) substrate.<br />
Si overgrowth leads to the formation <strong>of</strong> epitaxial,<br />
(111) oriented silicon.<br />
Novel tunneling devices?
Epita Epitaxial<br />
xial Growth <strong>of</strong> Heterolayers
Pseudomorphic Growth (Strained Layer)<br />
compressive<br />
strained SiGe<br />
(pseudomorphic)<br />
Si substrate
Relaxed Layer ( (Misfit Misfit Dislocations)<br />
relaxed SiGe<br />
mf dislocation<br />
Si substrate
Virtual Substrate (Strained Strained Si Layer Layer)<br />
tensile<br />
strained Si<br />
Relaxed<br />
SiGe<br />
Si Substrate
Band Gap for Strained SiGe and silicon<br />
Band Gap (eV)<br />
at 90 K<br />
1.2<br />
1.1<br />
1.0<br />
0.9<br />
0.8<br />
Strained SiGe<br />
on Si<br />
Relaxed SiGe<br />
Strained Si<br />
on relaxed SiGe<br />
0.7<br />
0.0 0.2 0.4 0.6 0.8 1.0<br />
Ge Concentration<br />
Strain reduces the band gap
SiGe Valley Splitting: Conduction Band<br />
Strained SiGe on Si<br />
[001]<br />
[100]<br />
[010]<br />
[001]<br />
Unstrained Si<br />
6-fold<br />
degenerated<br />
[010]<br />
[100]<br />
Strained Si on<br />
relaxed SiGe<br />
[001]<br />
Intervalley scattering can be reduced<br />
Increase in carrier mobility<br />
[010]<br />
[100]
Strain and Carrier Mobility<br />
Normalized Mobility<br />
2,5<br />
2,0<br />
1,5<br />
NMOS<br />
PMOS<br />
1,0<br />
0 10 20 30 40<br />
Ge Concentration (%)<br />
<strong>of</strong> the Substrate<br />
Strained Si on relaxed SiGe
State State-<strong>of</strong> State-<strong>of</strong>-the-Art<br />
<strong>of</strong>-the the-Art Art<br />
CMOS with<br />
• 50 nm Gate length<br />
• Strained Silicon<br />
• 1.2 nm SiO 2<br />
• Nickel silicide<br />
1.2 nm<br />
1.2nm<br />
SiO 2<br />
silicide<br />
Strained Si<br />
INTEL: IEDM Dez. 2002
Scaling will go on
Moore’s “ “Law “Law” Law”<br />
<strong>The</strong> number <strong>of</strong> transistors per chip<br />
doubles every 18 months<br />
Execution to Moore’s Law is<br />
becoming more material dependent<br />
Further scaling will reach<br />
physical limits
Material Complexity is Compounding<br />
Number <strong>of</strong> New Fab Materials<br />
Compared to the 0.35 micron Baseline<br />
50<br />
45<br />
40<br />
35<br />
30<br />
25<br />
20<br />
15<br />
10<br />
5<br />
0<br />
0.25 micron<br />
0.18 micron<br />
0.13 micron<br />
0.13 micron<br />
(300 mm)<br />
Revolutionary:<br />
Characterized by or<br />
resulting in radical change.<br />
Evolutionary:<br />
A gradual process in which<br />
something changes into a<br />
different and usually more<br />
complex or better form.<br />
Source: INTEL
Evolutionary Changes<br />
CMP: Composite abrasive slurries<br />
SILICON: Double-Sided Polished<br />
PHOTORESIST: 193 nm<br />
DIELECTRICS: Fluorine- & Carbon-Doped SiO 2<br />
METALS<br />
– Ta Barrier<br />
– Salicides<br />
– Target Assembly
Revolutionary Changes<br />
LOW K DIELECTRICS<br />
– Spin-on polymers<br />
– Porous materials<br />
HIGH K GATE DIELECTRICS<br />
– Metal ox ides<br />
– Mixed silicates<br />
METALS<br />
– Dual Damascene Copper<br />
– Advanced Bump Metallurgy instead <strong>of</strong> bonding<br />
– Atomic Layer Deposition
Revolutionary Changes<br />
CHEMICAL-MECHANICAL POLISHING (CMP)<br />
– Fixed & bonded abrasive pads<br />
– Abrasive-free slurries<br />
SILICON<br />
– Isotopically-enriched Si (28)<br />
– Si on Insulator (FD or PD-SOI)<br />
PHOTORESIST<br />
– 157 nm<br />
– EUV<br />
CARRIER: FOUP
Power Density Continues to Get Worse<br />
Watt/cm 2<br />
1000<br />
100<br />
10<br />
1<br />
1985<br />
P446<br />
P648<br />
1990<br />
P650<br />
P852<br />
1995<br />
P854<br />
P856<br />
2000<br />
P858<br />
P860<br />
2005<br />
P1262<br />
P1264<br />
2010
Future Drivers<br />
Logic process technologies are driven by<br />
3 key technology areas:<br />
Transistor performance<br />
– Gate oxide quality, channel mobility, …<br />
– Leakage currents<br />
Patterning / etching <strong>of</strong> nanometer lines<br />
Low RC interconnects
Lithography: Yesterday, Today, and Tomorrow
Bridging the SubWavelength Gap
CPU Multi Multi-layer layer Metal Increase Trend<br />
# <strong>of</strong> Metal Layers<br />
8<br />
7<br />
6<br />
5<br />
4<br />
3<br />
2<br />
1<br />
0<br />
1980-2µ<br />
1984-1.5µ<br />
1987-1.0µ<br />
1990-0.8µ<br />
1993-0.6µ<br />
1995-0.35µ<br />
1997-0.25µ<br />
1999-0.18µ<br />
2001-0.13µ<br />
2003-0.09µ
0.5µm<br />
P-WELL P-W WELL ELL<br />
N-WEL WEL L<br />
P+ Substrate<br />
Epi<br />
P-WELL P-W WELL ELL<br />
N-WEL WEL L<br />
Epi
RC Delay<br />
Assumption<br />
Assumption: : two parallel<br />
interconnects will be<br />
treated as a capacitor<br />
C = LW K ox ε 0 /t ox<br />
R = ρ met L/W t met<br />
t met<br />
RC ~ ρ met K ox L²/t ox t met<br />
Only a problem for long interconnects<br />
interconnects!<br />
t ox
RC Delay<br />
Strategies<br />
Strategies:<br />
RC ~ ρ met K ox L²/t ox t met<br />
- lowest possible resistivity<br />
- thick interlayer dielectric<br />
- thick metal layer<br />
Limited by global design issues<br />
Interlayer Interlayer with low K ox<br />
(low low-K K dielectrics<br />
dielectrics, , e.a. polymers<br />
polymers)
Groups <strong>of</strong> Low Low-K Materials<br />
<strong>Red</strong>ucing dielectric constant k<br />
Decreasing polarity<br />
1<br />
Decreasing density<br />
Groups <strong>of</strong> materials Bulk dielectric constant Deposition<br />
SiO 2 3.9 - 4.3 K CVD<br />
Fluorinated oxide1 3.4 - 3.9 low-K CVD<br />
Organosilicate glass1,2 2.5 - 3.0 low-K CVD<br />
Organic polymer 1 2.5 - 3.0 low-K CVD/SOD<br />
Porous organic polymer 1,2 2.0 - 2.5 ultra low-K SOD<br />
Porous organic polymer 1,2 1.5 - 1.9 extreme low-K SOD<br />
2
Calculated Delay vs. Technology Generation<br />
Delay (ps)<br />
45<br />
40<br />
35<br />
30<br />
25<br />
20<br />
15<br />
10<br />
5<br />
0<br />
Gate Delay<br />
Cu + low-K<br />
Al + SiO 2<br />
Total (Cu + low-K)<br />
Total (Al + SiO )<br />
2 600 500 400 300 200 100<br />
Pitch Size (nm)<br />
Al: 3.0 µΩcm<br />
Cu: 1.7 µΩcm<br />
SiO2: κ = 3.9<br />
Low K: κ = 2.0<br />
Al & Cu: 0.8 µm thick<br />
50 µm long<br />
Interconnect optimized circuit design will be needed
Cost <strong>of</strong> a Chip Factory<br />
“Second Moore’s Law”<br />
Fab cost doubles every 3 years
Worldwide <strong>Semiconductor</strong> Sales<br />
1975 1975-2005<br />
2005<br />
$Billions<br />
250<br />
200<br />
150<br />
100<br />
50<br />
0<br />
1975<br />
1977<br />
1979<br />
1981<br />
1983<br />
1985<br />
1987<br />
1989<br />
1991<br />
1993<br />
1995<br />
1997<br />
1999<br />
2001<br />
2003*<br />
2005*<br />
Source: SIA Fall 2002 Forecast<br />
* Forecast
$35<br />
$30<br />
$25<br />
$20<br />
$15<br />
$10<br />
$5<br />
$0<br />
Intel<br />
Toshiba<br />
NEC<br />
Samsung<br />
TI<br />
Top 22 Chip Manufacturers 2000<br />
STMicro<br />
Final 2000 numbers<br />
from Dataquest*<br />
Motorola<br />
Hitachi<br />
Infineon<br />
Micron<br />
Hyundai<br />
Philips<br />
Mitsubishi<br />
Fujitsu<br />
TSMC*<br />
Lucent<br />
AMD<br />
IBM<br />
'98 ($B)<br />
'99 ($B)<br />
'00 ($B)<br />
Source: Dataquest, *TSMC and UMC annual reports — the latter don't sell chips into the market<br />
Matsushita<br />
Sony<br />
Sharp<br />
UMC*
<strong>The</strong> Need for Globalization<br />
manufacturer<br />
manufacturer<br />
90’s 21 st Century<br />
Technology<br />
Economics<br />
Global<br />
<strong>Semiconductor</strong><br />
Industry
Mega Business Trends<br />
Cost <strong>of</strong> Fab, instead <strong>of</strong> technology<br />
breakthrough, impacts global industry food<br />
chain<br />
– size matter; CPU, DRAM alliance<br />
– Foundry fab (TSMC and others)<br />
Migration to Developing Country will<br />
accelerate<br />
– Foundry to Asia (Taiwan, China…)<br />
– Fabless design to Taiwan, Israel, Russia, India…
Asia Pacific Leads<br />
$Billions<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
Regional <strong>Semiconductor</strong> Market<br />
2001 2002* 2003* 2004* 2005*<br />
Americas Europe Japan Asia Pacific<br />
Source: SIA Fall 2002 Forecast<br />
*2002 Grow th Rates
Growth <strong>of</strong> the Internet<br />
Mill.<br />
10000<br />
1000<br />
100<br />
World population<br />
TV & Telephone<br />
PC<br />
“Internetter Internetter”<br />
10<br />
‘95 ‘96 ‘97 ‘98 ‘99 ‘00 ‘01 ‘02 ‘03 ‘04
Wireless Internet<br />
Wireless (<strong>of</strong> course!)<br />
– But much more than wireless access to the net<br />
Personal<br />
– Accessed by personalized, handheld terminals<br />
– “Wearable computers”<br />
Location aware<br />
– Information & services you need where you happen to be<br />
Context aware<br />
– You need a ticket at the train station<br />
Transaction based
Web Tablet
Nanoelectronics
Other New Concepts (here: Memories)
Visions<br />
Integration <strong>of</strong> Opto and Microelectronics on one Chip
New Device Concepts<br />
Gate Oxide<br />
Body<br />
Drain<br />
Silicon Film<br />
Buried Oxide<br />
Substrate<br />
Poly Gate<br />
Source<br />
Body<br />
BOX<br />
Source Drain<br />
Source<br />
Gate<br />
Drain<br />
Si fin - Body!
V S<br />
Beyond the classical FET<br />
1) MOSFET<br />
V S<br />
V G<br />
2) SBFET<br />
V G<br />
V D<br />
V D<br />
3) CNTFET<br />
4) Molecular transistors?<br />
V G<br />
V S<br />
V D
Scaling will reach physical limits….<br />
10 nm MOSFET Molecule<br />
or<br />
?
Carbon Nanotubes
Summary<br />
Innovations on all levels are needed for future progress<br />
– Materials (high-K, low-K, new metals, SOI,…)<br />
– Device concepts (3D integration, …)<br />
– IC architectures (interconnect optimized design, …)<br />
<strong>The</strong> „classica l“ microelectronic (CMOS, …) is getting<br />
closer to its limits<br />
– Material limits<br />
– Technical limits<br />
– Economical limits (too expensive)<br />
Nanoelectronics<br />
– Devices with small number <strong>of</strong> electrons<br />
– Molecular approaches<br />
– Fabrication by self organization<br />
– Various quantum effects (spintronic, quantum computing)