Robert Chau ICSICT 101904
Advanced CMOS Transistors
in the Nanotechnology Era
for High-Performance, Low-Power
Logic Applications
Robert Chau
Intel Fellow
Director of Transistor Research
and Nanotechnology
Intel Corporation
Oct 19, 2004
(2)
Content
•
Introduction
•
State-of-the-art Si nanotechnologies for
advanced CMOS transistors
–
High-K, Metal-gate, Strain, Non-planar Tri-gate
•
Emerging nano-electronic materials and
devices
for future logic applications
–
III-V, Carbon Nanotubes, Semiconductor
Nanowires
•
Challenges and Opportunities
•
Summary
(3)
Technology Node
0.5µm
0.35µm
0.25µm
0.18µm
0.13µm 90nm
65nm
45nm 30nm
Transistor Physical Gate
Length 130nm
70nm
50nm
30nm
20nm
15nm
1995
2005
1990
2000
2010
0.01
0.10
1.00
Micrometer
Nanotechnology
10
100
1000
Nanometer
Transistor Scaling
• Transistor physical gate length will reach ~15nm before
end of this decade, and ~10nm early next decade
3
(4)
Transistor Scaling and Research Roadmap
Transistor Scaling and Research Roadmap
4
Gate
LG= 10nm
LG= 10nm
20nm Length (Development) 25 nm 15nm 15nm Length 15nm Length (Research) (Research) 65nm Node 2005 45nm Node 2007 90nm Node 2003 32nm Node
2009 22nm Node
2011 10nm Length 10nm Length (Research) (Research) C
C--nanotubenanotube Prototype
Prototype
(Research)
(Research) NanowireNanowire
Prototype
Prototype
(Research)
(Research)
5 n m
5 n m
5nm
2015-2019
Research
50nm Length (Production) 30nm Length (Development)Drain
Source
Source
III-V Device Prototype (Research)S G D
Epi III-V Non-planar Tri-Gate Architecture Option 30nm Uniaxial Strain
SiGe S/D PMOS
High-K & Metal-Gate Options
1.2nm Ultra-thin SiO2
(5)
State-of-the-Art Si Nanotechnologies
•
Gate Dielectric Technology
– Ultra-thin 1.2 nm nitrided gate oxide (implemented
in 90nm technology node)
– New high-K/metal-gate stack (key option for 45nm
node)
•
Strained Si Technology
• Uniaxial strain (implemented in 90nm node) • Biaxial strain
•
Non-planar Tri-gate Transistor Architecture
(
option for 45nm, 32nm node and beyond)•
Si transistor is becoming less silicon
– SiGe S/D, metal gate electrodes, metallic high-K etc 5
(6)
High-K/PolySi Transistors
1.E-08 1.E-07 1.E-06 1.E-05 1.E-04 1.E-03 1.E-02
0 0.2 0.4 0.6 0.8 1 1.2 Vg (V)
Id
(
A
/µ
m)
Vd = 1.3V Lg = 110nm
PolySi/High-K Toxe = 17A
PolySi/SiO2 Toxe = 20A
•
High-K/polySi transistors suffer from high VTH,degraded channel mobility and poor drive performance
High-K / Poly-Si
0
100 200 300 400 500
0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 Electric Field (MV/cm)
In
versio
n
Electro
n
Mo
bility
(cm2/Vs)
Universal Mobility
SiO2/Poly-Si
6
(7)
High-K and PolySi are Incompatible
O M
O O O O
M M M
O M
O O O O
M M M
O O O O O O O O
O M
O O O O
M M M
O M
O O O O
M M M
M
O M
O O O O
M M M
O M
O O O O
M M M
M Si
Si Si Si Si Si Si
Si Si
Si
Si Si Si Si Si Si Si Si Si Si
Si
Si Si Si Si Si Si Si Si Si Si
Si
Si Si Si Si Si Si Si Si Si Si
M Si Si Si Si Si
Poly Si
Interface
High-K
M = Zr, Hf
Defect
•
Defect formation at the polySi-high-K interface
•
1 defect out of 100 surface atoms to pin Vth
7
(8)
Phonon Scattering Limits Channel
Mobility in High-K/PolySi Transistors
1.0E-05 1.5E-05 2.0E-05 2.5E-05 3.0E-05 3.5E-05 4.0E-05 4.5E-05
0.1 0.3 0.5 0.7 0.9 1.1 1.3 1.5
E-Field (MV/cm) d(1/ueff)/dT High-K/PolySi SiO2/PolySi Phonon scattering E-Field µ 0 1 > ∂ ∂ T PH µ 0 1 < ∂ ∂ T Coul µ 0 1 = ∂ ∂ T SR µ
µph ↓ T ↑
µCoul ↑ T ↑
µSR~ const
Coulombic Phonon Surface
Roughness
SR ph
Coul
eff µ µ µ
µ
1 1
1
1 = + +
8
(9)
Metal Gate Screens Surface Phonon Scattering
and Improves Mobility in High-K Transistors
0 200 400 600 800 1000 1200
0 0.5 1 1.5
Transverse Electric Field, Eeff ( MV/cm)
Surface Phonon Limited Mobility
(cm
2 /V.s)
471
P860
W019-BKM
SiO2 + Poly-Si HfO2 + PolySi HfO2+Metal Gate
T = 25 C
High-K/PolySi SiO2/PolySi
High-K/Metal-gate
9
(10)
Metal Gate Electrodes with the “Right” Work
Functions are Required for Correct Transistor V
THNDK
SDK
-1.1 -1.0 -0.9 -0.8 -0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0.0 0.1
N+poly P+pol
y
P-metal
N-metal Metal A Metal B Metal C Metal D Metal E Metal F Metal G Metal H Metal I Metal J Gate Electrode Materials
Transistor Flatband
Voltage
(V)
P-type Metal on High-K
N-type Metal on High-K
N+ PolySi/SiO2
P+ PolySi/SiO2
Mid-gap Metal on High-K
(11)
High-Performance High-K/Metal-Gate CMOS
Transistors
(Thin Toxe, Correct V
TH, High Mobility
and Low Gate Leakage)
1E-09 1E-08 1E-07 1E-06 1E-05 1E-04 1E-03 1E-02
-1.4 -1 -0.6 -0.2 0.2 0.6 1 1.4
GATE VOLTAGE (V)
DR
A
IN CUR
R
ENT (A
/µ
m)
NMOS PMOS
Lg= 80 nm
Toxe= 14.5 Å
|Vds| = 0.05, 1.3 V
1E-09 1E-08 1E-07 1E-06 1E-05 1E-04 1E-03 1E-02
-1.4 -1 -0.6 -0.2 0.2 0.6 1 1.4
GATE VOLTAGE (V)
DR
A
IN CUR
R
ENT (A
/µ
m)
NMOS PMOS
Lg= 80 nm
Toxe= 14.5 Å
|Vds| = 0.05, 1.3 V
0.0E+00 2.0E-04 4.0E-04 6.0E-04 8.0E-04 1.0E-03 1.2E-03 1.4E-03 1.6E-03 1.8E-03
-1.4 -1 -0.6 -0.2 0.2 0.6 1 1.4 Vds (V) Id ( A /µ m ) NMOS PMOS
Lg = 80nm Toxe, inv = 14.5Å |Vgs|= 0V to 1.3V
•
High-K/Metal-K is a key option for the 45nm node11
(12)
Channel Mobility Enhancement using
Uniaxial Strain (Implemented in 90nm node)
SiGe
SiGe
PMOS
Uniaxial, Compressive Strain in Si Channel in PMOS using SiGe S/D
Uniaxial, Tensile Strain in Si
Channel in NMOS using Silicon Nitride Cap
NMOS
High Tensile Silicon Nitride Film
12
(13)
13
Channel Mobility Enhancement Using
Biaxial Strain (PMOS Example)
Strained SiGe channel
Si
TiN / High-K gate stack
Strained SiGe channel
Si
TiN / High-K gate stack
Strained SiGe channel
Si
TiN / High-K gate stack High-K/Metal-Gate Stack
Strained SiGe Channel
Silicon Substrate
■ ● ◆
High-K/MG on SiGe(30% Ge) High-K/MG on SiGe(25% Ge) High-K/MG on SiGe(20% Ge) High-K/MG on Si
SiO2 Universal Mobility
Si Strained SiGe (Biaxial
Compressive)
Si SiGe
•
Enhancement in both
low-field and high-field
channel mobility
(14)
Si
W Si
TSi LG
W Si
TSi LG
Non-Planar Transistors
TSi LG
W Si
TSi LG
W Si
ISOLATION
Double Gate (e.g. FINFET) Non-Planar Tri-Gate
(15)
Non-Planar Tri-Gate Transistor
Si Planar
Si Non-planar Tri-gate
NMOS
Si Planar
NMOS
Si Tri-gate
15
•
Si planar transistors becoming difficult to scale•
Tri-gate architecture improves electrostatics significantly and extends transistor scalability•
Tri-gate is a key device option for 32nm node and beyond(16)
Tri-Gate Transistor Architecture for
32nm Node and Beyond
PMOS
Si Planar
Si Non-planar Tri-gate
PMOS
Si Planar
Si Non-planar Tri-gate
16
•
Tri-gate architecture shows significantly improved device electrostatics and short-channel performance overconventional planar architecture
(17)
Nanotechnology Research
Lg = 10 nm
(a)
Lg = 10 nm Gate
Source Si body Drain Gate Source Drain Source CNT Single -wall D = 1.4 nm
Gate (Pt) Drain
(Pd)
Lg = 75 nm
(d)
Source
CNT
Single -wall D = 1.4 nm
Gate (Pt) Drain
(Pd)
Lg = 75 nm
(d)
Source
CNT
Single -wall D = 1.4 nm
Gate (Pt) Drain
(Pd)
Lg = 75 nm
III-V Gate Drain Source Source (c) Multi epitaxial layers Gate Drain Source Source (c) Multi epitaxial layers Gate Drain Source Source Multi epitaxial III-V layers
5 nm 5 nm
2.0 nm High-K Gate
5.0 nm Si Nanowire
5 nm 5 nm
2.0 nm High-K Gate
5.0 nm Si Nanowire
• Semiconductor
Nanowires
(Si, SiGe, Ge etc)
• Carbon Nanotube • III-V Transistors
17
(18)
18
Intrinsic gate delay CV/I for PMOS
0.1 1 10 100 1000
1 10 100 1000 10000
GATE LENGTH [nm]
G
A
T
E
D
E
L
A
Y
[p
s
]
Si MOSFETs CNTFETs Si Nanowires PMOS
• CNT shows significant p-ch CV/I improvement over Si
– CNT has >20X higher effective p-ch mobility than Si
• Si nanowires do not show improvement over Si
(19)
19
• n-channel CNT not as well established as p-channel CNT
• III-V (e.g. InSb) devices show significant CV/I improvement over Si
– III-V devices have >50X higher effective n-ch mobility than Si
– III-V devices operated at low VCC = 0.5V
• Scalability of III-V devices to shorter Lg remains to be demonstrated
Intrinsic gate delay CV/I for NMOS
(20)
20
III-V Transistors for Low Vcc
GATE DRAIN DRAIN SOURCE III-V 0 20 40 60 80 100 120 140 160 180
1 10 100 1000
Power Dissipation (mW/mm)
Cutoff Frequency, fT (GHz)
InSb Vds=0.3V InSb Vds=0.5V InSb Vds=0.6V InSb Vds=0.7V Si Vds=0.5V Si Vds=0.7V Si Vds=1V Si Vds=1.2V III-V FETs (Lg~200nm) Si FETs (Lg~80nm) 5-10X Lower Power Dissipation 0.5V 1.2V
Robert Chau, Intel, ICSICT 2004
0.3V
T eff
m
v
f
L
g
WL
C
I
WLV
C
I
CV
π
2
1
00
=
=
=
(21)
Device Evolution and Process Challenge
21
Planar Si
Source Drain
Gate
Tri-gate
CNT/Nanowire
GATE DRAIN
DRAIN SOURCE
Epitaxial III-V
III-V
Bottom-up Approach
•
Chirality issues•
Positioning issues(required >10 billion gates)
32nm Node (2009)
Conventional Processing (being done in 300mm Fabs)
•
Top-down Approach – std litho and etch•
Integration with Si?(22)
Summary
22
•
Through Si breakthroughs and innovations,
Si CMOS transistor scaling will continue
through middle of next decade
•
Future logic transistor scaling and
performance require research on new
device structures, new materials, new
process technologies, and new integration
schemes
•
Emerging nanoelectronic devices show
both challenges and opportunities for
future logic transistor applications
(1)
Nanotechnology Research
Lg = 10 nm (a)
Lg = 10 nm Gate
Source Si body Drain Gate Source Drain Source CNT Single -wall D = 1.4 nm
Gate (Pt) Drain
(Pd)
Lg = 75 nm
(d)
Source
CNT
Single -wall D = 1.4 nm
Gate (Pt) Drain
(Pd)
Lg = 75 nm
(d)
Source
CNT
Single -wall D = 1.4 nm
Gate (Pt) Drain
(Pd)
Lg = 75 nm
III-V Gate Drain Source Source (c) Multi epitaxial layers Gate Drain Source Source (c) Multi epitaxial layers Gate Drain Source Source Multi epitaxial III-V layers
5 nm
5 nm
2.0 nm High-K Gate
5.0 nm Si Nanowire
5 nm
5 nm
2.0 nm High-K Gate
5.0 nm Si Nanowire
• Semiconductor
Nanowires
(Si, SiGe, Ge etc)
(2)
Intrinsic gate delay CV/I for PMOS
0.1 1 10 100 1000
1 10 100 1000 10000
GATE LENGTH [nm]
G
A
T
E
D
E
L
A
Y
[p
s
]
Si MOSFETs CNTFETs Si Nanowires
PMOS
• CNT shows significant p-ch CV/I improvement over Si
– CNT has >20X higher effective p-ch mobility than Si
(3)
• n-channel CNT not as well established as p-channel CNT
• III-V (e.g. InSb) devices show significant CV/I improvement over Si – III-V devices have >50X higher effective n-ch mobility than Si
– III-V devices operated at low VCC = 0.5V
• Scalability of III-V devices to shorter Lg remains to be demonstrated
(4)
III-V Transistors for Low Vcc
GATE DRAIN DRAIN SOURCE III-V 0 20 40 60 80 100 120 140 160 1801 10 100 1000
Power Dissipation (mW/mm)
Cutoff Frequency, fT (GHz)
InSb Vds=0.3V InSb Vds=0.5V InSb Vds=0.6V InSb Vds=0.7V Si Vds=0.5V Si Vds=0.7V Si Vds=1V Si Vds=1.2V III-V FETs (Lg~200nm) Si FETs (Lg~80nm) 5-10X Lower Power Dissipation 0.5V 1.2V 0.3V T eff
m v f
L g WL C I WLV C I CV π 2 1 0
0 = = =
(5)
Device Evolution and Process Challenge
Planar Si
Source Drain Gate
Tri-gate
CNT/Nanowire
GATE DRAIN
DRAIN SOURCE
Epitaxial III-V
III-V
Bottom-up Approach
• Chirality issues
• Positioning issues
(required >10 billion gates)
32nm Node (2009)
Conventional Processing (being done in 300mm Fabs)
• Top-down Approach – std litho and etch
(6)
Summary
• Through Si breakthroughs and innovations,
Si CMOS transistor scaling will continue through middle of next decade
• Future logic transistor scaling and
performance require research on new device structures, new materials, new
process technologies, and new integration schemes
• Emerging nanoelectronic devices show
both challenges and opportunities for future logic transistor applications