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Transcript of 7 Jan - CMOS Devices - Navakant.pdf
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8/14/2019 7 Jan - CMOS Devices - Navakant.pdf
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Navakanta Bhat
CMOS Devices
Process Integration
Navakanta Bhat
ProfessorCentre for Nano Science and Engineering (CeNSE)
Dept. of Electrical Communication Engineering,
Indian Institute of Science, Bangalore
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Navakanta Bhat
Outline
CMOS Technology and Design Objectives
Isolation
Wells
Gate Stack
Junctions
Interconnects
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The Integrated Circuit Food Chain
Optimization across all the domains is necessary
Process Technology
Device Physics
Circuit Design
System Architecture
Application
Domain
Technology
Domain
CAD and Modeling
Computational State Variable
Digital Architecture
Boolean Logic
CMOS
Charge
Silicon
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What is in a IC Chip ?A large ensemble of transistors connected appropriately
through multilevel metal interconnection lines
Every thing should be made as simple as possible,but no simpler! Albert Einstein
INTEL IBM
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CMOS : NMOS + PMOS
switch modellay outschematic
Gate
Drain
Source
CMOS
IDcross section
NMOSFET
n n
Silicon
G
p-well
oxide
VG
Vth
p p
Silicon
G
n-well
oxide
PMOSFET
Vth
CMOS
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Performance Metrics in CMOS
P=CL*Vdd2*fD= CL*Vdd/Ids
CL
IN OUT
Vdd
Ids
Ids
CL , total capacitance at the switching node
Vdd , supply voltage
f , switching frequency
Ids , charging or discharging current
INVERTER Gate CapacitanceJunction Capacitance
Interconnect Capacitance
CAPACITANCE IS INERTIA
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Vt-Vdd design planeNormalized delay
Vt/Vdd0.4
Delay increases significantly for Vt/Vdd > 0.4
Pactive (Pac) = CVdd2
fPstandby (Psb) = WVddIoff
Vt
Vdd
Psb
Pac
Delay
Delay and Power are the only trade-off points for digital design
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Transistor Design Metrics
Ioff
Ion Ion
CDC Metric AC Metric
BETTERDESIGN
BETTERDESIGN
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Transistor design methodology for Digital CMOS
Design parameters: L, Vdd, Tox, N, Xj
S/D engineering
Channel engineering
Choice of materials and processes
Circuit characteristics:
Delay (Vt/Vdd)Active power (Vdd)
Standby power (Vt)
Hot carrier reliability
Vdd, L, N
Gate oxide reliability
Vdd, Tox
System compatibility
Vdd
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Constant Electric Field Scaling
Primary scaling factors:
Tox, L, W, Xj (all linear dimensions) 1/K
Na, Nd (doping concentration) K
Vdd (supply voltage) 1/K
Derived scaling behavior of transistor:Electric field 1
Ids 1/K
Capacitance 1/K
Derived scaling behavior of circuit:Delay (CV/I) 1/K
Power (VI) 1/K2
Power-delay product 1/K3
Circuit density (
1/A) K2
Technology scaling
Scaling factor K > 1
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Technology Life cycle
Source : ITRS 2007
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Worldwide Wafer Production across Technologies
Source : ITRS 2007
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Microelectronics to Nanoelectronics
1960 2020
New Materials and
Device structuresSilicon CMOS
2010
45nm 15nm
Nano-scale building blocks and Giga-scale Integration!
Channel quantization
Quasi ballistic transport
SCALiNG
Gate tunneling
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ITRS Projections
Year of Production
2007 2010 2013 2016 2019 2022
Technology Node (nm) 65 45 32 22 16 11
Printed Gate Length (nm)
Physical Gate Length (nm)
42
25
30
18
21
13
15
9
11
6.3
7.5
4.5
Wafer diameter (inch) 12 12 18 18 18 18
Number of masks required for
fabrication of Microprocessor
33 35 37 37 39 39
Number of Transistors inMicroprocessor (billion)
1.1 2.2 4.4 8.8 17.7 17.7
Number of interconnect wiring
levels in the Microprocessor
15 16 17 17 18 18
Number pins for packagedMicroprocessor chip
1088 1450 1930 2568 3418 3760
Operating voltage (V) 1.1 1.0 0.9 0.8 0.7 0.7
Microprocessor frequency, GHz 9.3 15.1 23 39.7 62.4 73.1
Chip power dissipation (Watts) 189 198 198 198 198 198
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ISOLATION MODULE
LOCal Oxidation of Silicon (LOCOS)
Shallow Trench Isolation
SiO2 is used isolate two transistors
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LOCOS Isolation
~10nm Pad SiO2Dry oxide
Si
~15nm Si3N4LPCVD
Si
Active Litho,
Dry etch
Si
~500nm Field SiO2Wet oxide
Si
Strip nitride, oxideWet etch
Si Si
Scalability is an issuedue to Birds beak
Not suitable for < 250nmComment on Wafer Type
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Shallow Trench Isolation
~10nm Pad SiO2Dry oxide
Si
~15nm Si3N4LPCVD
Si
Active Litho,Dry etch
~350nm depth
Si
Si
Liner oxide (~10nm)HDPECVD trench fill
TEOS chemistry
Si
Chemical MechanicalPolishing, HF dip,
Nitride strip
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Well Module
What are the requirements forNano MOSFET Design ?
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SHORT
CHANNEL
EFFECTS
Nano MOSFET : Design Issues
S D
GS D
G
Leakage current
L (m)
Vt
~1m
Drain Induced
Barrier Lowering (DIBL)
Vt roll-off
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How do you minimize SCE?
Screen the electric field
Increase Substrate Doping Concentration
Increased impurity scattering
Degradation of sub-threshold slope
Increased junction capacitance
Minimize coupling volumeDecrease source/drain depth
Increased source/drain resistance
Junction spiking
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Transistor Structure Requirement
Y
X
Pocket halo
Super steep retrograde
channel
spacer
n+n+
p-well
gate
oxide
source drain
Short channel effects are controlled by shallow extensions,
pocket halos and super steep retrograde channel
Na
L0 Y
Na
0 X
Deep S/D and
Shallow Extension
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Other Requirements
Si
Prevent DeepPunch Through
Account for highfields at trenchcorner
Adjust Vt
USE CHAIN OF IMPLANTS
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Well Implant Chain
Boron ~ 200 KeV, 1012 1013 /cm2
Boron ~100 KeV, 1012 1013 /cm2
Boron ~50 KeV, 1012 1013 /cm2
Boron ~ 15 KeV, 1012 1013 /cm2
Indium ~ 120 KeV, 1012 1013 /cm2
Phosphorus ~ 600 KeV, 1012 1013 /cm2
Phosphorus ~300 KeV, 1012 1013 /cm2
Phosphorus ~ 50 KeV, 1012 1013 /cm2
Phosphorus ~ 15 KeV, 1012 1013 /cm2
Antimony ~ 150 KeV, 1012 1013 /cm2
P-Well N-Well
Multiple Vt Technology
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Gate Stack Module
SiO2, Dual Polysilicon Gate
High-K, Metal Gate
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Polysilicon Gate stack
Si
Phase Shift Litho
Resist Trim
Si
Poly Etch
Si
i-PolySiliconLPCVD
Si
Dry, 800C, O2+N2Nitridation
Si
RCA Clean
NBTI Reappears!
Comment on Dual
Gate technology
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Why High-K and Metal Gate
Increasing gate resistance
for short channel device
Activation of poly-Si
Direct Tunneling current
High K Metal Gate Gate stack
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High-K Metal Gate Gate stack
Si
RCA Clean
Si
PVD HfO2
Si
i-PolySiliconLPCVD
Si
Phase Shift Litho
Resist Trim
Si
Poly Etch
DISPOSABLE GATE PROCESS
Dispose -off polySi after
ILD0 and fill the gate
trench with dual metalgate materials
Ensures Self Aligned
transistor
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Junction Module
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NMOS Halo and Extension
Si
Si
Arsenic, 0o tilt, ~1014, 5KeV
Si
Boron, 45o
tilt, ~1012
, 15KeVNMOS S/D Litho
STORY #1:
Shadow
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PMOS Halo and Extension
Si
Phosphorus, 45o
tilt, ~1012
, 35KeV
Si
BF2, 0o tilt, ~1014, 3 KeV
Si
PMOS S/D Litho
STORY #2
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Spacer Formation
Deposit 10nm Oxide, 40nm nitride
What about Oxide spacers ??
Boron segregation degrades PMOS
Si
Anisotropic nitride etchSi
STORY #2: Cgd
Comment on offset spacers for extension
Deep S/D Implant and Anneal
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Deep S/D Implant and AnnealNMOS S/D Litho
Arsenic, 15 KeV, ~1015
Si
PMOS S/D Litho
Boron, 5 KeV, ~1015
Si
Si
RTA
Trade off between poly depletion,versusJunction depth & Boron Penetration
Sili id F ti
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Silicide Formation
PVD Metal
RTA
ETCH METAL
S D
G
Parasitic Channel Resistance
Si
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Interconnect Module
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ILD0 , Contact and Metal1
Si
ILD0 CVDContact Litho & Etch
W CVD and CMP
Aluminum PVDMetal Litho & Etch
Forming gas anneal
Same process continues for Via1, Metal2, Via2, Metal3
STORY #3: Yield
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Interconnect delay in Nano CMOS
Delay
0.50.350.250.18
Technology node (m)
Intrinsic gate delay
Interconnect delay
Gate delay decreases due to decrease in gate capacitanceInterconnect delay increases due to decreasing metal line width
and increasing intra-metal coupling capacitance
Interconnects are no longer afterthought in Nano CMOS
Copper Interconnects
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Copper Interconnects
ILD CVD (thickness for via and metal)
Litho Via holes and etch via hole
Litho Metal trenches and etch metal trenchCopper Electroplating and CMP
Si
Dual Damascene Process
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Beyond Bulk Silicon CMOS
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SOI CMOS ?
500mInsulator
SOI Bulk
Si wafer
Si film
(10-100nm)
Devices are built on thin Si film (~100nm) on insulatorHandle Si wafer may be underneath the insulator (VLSI)
Insulator itself may form the rest of the substrate (Displays)
Si wafer
Partially Depleted SOI (PDSOI) versus Fully Depleted SOI (FDSOI)
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Components of node capacitance
CL=Cg + Cj + Ci
Cg = gate oxide capacitance
Cj = junction capacitance
Ci = interconnect capacitance
Cj= s A/Wd
s, permittivity of Si
Wd, depletion width
A , cross section area
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Other SOI specific effects
Fewer processing steps
Better isolation resulting in dense circuits
Drain current overshoot
Lower body effect
Absence of latch-up problem
Better sub-threshold slope
Threshold voltage (Vt) instability due to DC floating body effect
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SOI device delay
SOI results in at least 30% lower delay compared to bulk
The improvement is more pronounced at lower voltages
IBM data
SOI results in about 70% lower power for the same speed
IBM data
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SOI Power dissipation
SOI results in about 70% lower power for the same speed
IBM data
N d f M lti t FET
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Need for Multigate FETs
Alternate structures required for better gate control over the chann
- Double Gate, FinFET, Surround Gate
SiO2
n+ n+p
Increase in P type doping
with decreasing L results
inn+-p+ tunnel junction
Intels data
Fin FET
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Fin FET
H.S.P Wong, IBM Technical Journal
C OS ?
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CMOS with new materials ?
Germanium / GaAs / GaN ?
Graphene ?
Planar Technologies are Circuit designer friendlyas opposed CNT and other vertical transistors
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Germanium Schottky Barrier MOSFETs
Doped S/D
RovR
dp
R
extRscd
GateSpacer
Silicid
e
oxide
Metal
Advantages
Reduced series resistanceReduced short channel effects
Low thermal budget process Easy for Metal gate
Reduced process variability
*
* S-D Kim et al., Advanced Model and analysis of series resistance for CMOS scaling , IEEE TED, Vol. 49, No. 3, Marc
What about NMOS Schottky
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What about NMOS Schottky
Junction Transistors on Ge (or Si)
Technologically hard problem
Fermi level pinning in the bottomhalf of the band gap
For Si : Eg/3 above valence band edge
For Ge : Close to valance band edge
Schottky junctions on n-type Ge/Si are possible Schottky junctions on p-type Ge/Si have never been
very efficient
Ec
Ev
Ei
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Is it possible to passivate the interfaceand De-pin the Fermi level?
Literature on Sulphur passivationof III-V semiconductors exists
C S f
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Current State-of-the-art
Sulphur implantation: results in ohmiccontacts to both substrate types. Not
possible to produce Schottky Source/Drain. Passivation studies for Ge High-k
interface
done only for p-channel devices. N-channel
devices have proved very difficult to
passivate.
No studies exist on the effect of passivation
on Schottky Interface.
S l h P i i f G f
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Sulphur Passivation of Ge surface
Ge cleaned in HCl-HBr mixture to remove
native oxide.
Subsequently treated in Aqueous
Ammonium Sulphide ((NH4)2S ) solution
Passivation treatment carried out close toboiling point.
Al, Zr, Ta (Low work function)W, Ni, Pt (High work function)
XPS t di
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XPS studies
1210 1215 1220 1225 1230Binding Energy (eV)
Intensity(ArbitraryUnits)
Ge-SGe 2p3/2
160 165 170Binding Energy (eV)
Intensity
(ArbitraryUnits)
S 2p
25 30 35Binding Energy (eV)
Intensity
(ArbitraryUnits)
GeO2
S-pass.
HCl-HBr
Ge 3d5/2
Bare Ge
Native oxide peak disappears after cleaningand sulphur passivation
Sulphur peak is evident on Sulphur treatedWafers
Ge-S peak also apperas indicating that sulphur
Is chemically active on the surface
S h ttk t t G
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Schottky contact on p-Ge
Modification of behavior on p-Ge
-1 -0.5 0 0.5 1-60
-40
-20
0
20
40
60
Voltage(V)
J(A/cm
2)
Al pass.Zr pass.
Zr Un-pass.
Al Un-pass.
EV
EC
Eg
S h ttk t t G
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Schottky contact on n-Ge
Modification of behavior on n-Ge
-1 -0.5 0 0.5 1-60
-40
-20
0
20
40
60
Voltage(V)
J(A/c
m2)
Al Un-pass.Zr Un-pass.
Al pass.
Zr pass.
B i h i h d f i ti
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Barrier height trend after passivation
4.05 4.5 5 5.5 60
0.1
0.2
0.3
0.4
0.5
0.6
0.66
Un - passivated.
S - passivatedZr
Al
Ta
Ta
Zr
AlW
Ni
Pt
mvac
Electron
Barrie
r(Bn
)
Sulphur
passivation
results in almost ideal Schottky
behaviour
Ideal Theory
Arun
& Bhat
APL, 2010
S
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Summary
CMOS Process Integration
Isolation module
Well module
Gate stack module
Junction module
Interconnect module
CMOS Process Complexity continues to
increase with technology scaling
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Thank You