challenges in the future nanoelectronics · equipment & processes 50nm 35nm 35nm si pattern...
TRANSCRIPT
September 14, 2011
Jo-Won Lee1/Moon-Kyung Kim2
1 Dept. of Convergence Nanoscience, Hanyang University
2 Cornell University
Challenges in the Future Nanoelectronics
Comparison between Microprocessor & E. coli Source: Modified from M. Simpson & P. Cummings in ACS Nano, v5, p2425, 2011
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Through billions of years, nature has developed a self- assembling, selfduplicating, self-healing, adaptive processing unit that has 6 orders of magnitude higher memory density and 2 orders of magnitude higher computing capacity while utilizing 8 orders of magnitude less power. Required power for the robot as smart as the human
brain(20 Watt) :10-20 MW a small hydroelectric plant
Classification Microprocessor ( i7) Escherichia Coli
Memory Density 12 MB at 32nm (Cache)
= ~5X10-6 Mb/m2
9.2 Mb
= ~5 Mb/m2
# of Logic Gate ~1.2 B/240 mm2
= 5 logic gate/m2
~1,000
= ~500 logic gate/m2
Power Consumption 35 W
= ~3X10-8 W/m2
10-15 W
= 5X10-16 W/m2
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No Further Miniaturization for MOSFET
Technical Obstacles for Miniaturization
Variation in properties
and size - Unacceptable at nm scale
Lithography
- EUV is the final station
- What can be the next?
Scaling capability
- No solution for NAND Flash
below 10nm
Heat dissipation at nm
- Associated with raising and
lowering an energy barrier
of at least kβT
At present, below 10nm CMOS is very uncertain to manufacture.
- Functionality will be continuously increased following Moore’s law.
2005~2015 : Performance enhancements by new technology - Continued CMOS shrinking, Multicore chips, 3-D packaging, New memory, etc.
> 2015? : New device (Beyond CMOS)? → NRI’s Goal
4
1950 1960 1970 1980 1990 2000 2010
Bipolar CMOS
?
Start of Water Cooling
Year of Announcement
1940
Vacuum Tubes
14
12
10
6
4
2
0
8
Module
Heat Flu
x(w
atts/c
m2)
1947: Invention of Transistor
Why Look for a New Switch Source: Modified from Jeff Welser at INC5, UCLA, May 2009
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Prohibitive Cost Increase in Fab. Construction & Process R&D: EE Times, June 16, 2011
Year of Production
03~07 08~11 After 2012
Fab. Construction Cost (300mm )
~90 Toolsets necessary
Process R&D Cost
($ B
illio
n)
90~65nm 45~32nm 22~12nm 0
0.4
0.8
1.2
1.6
90~65nm 45~32nm 22~12nm
$0.3~0.4B
$0,6~0.9B
$1.3B
0
1
3
5
$2.5~3B
$3.5~4B
$4.5~6B
7
($ B
illio
n)
EUV tool costs hit $125M- EE Times, Nov. 19th 2010
Gradual Change in Nanofabrication Tech. Source: Modified from NISTEP Report, May, 2007
2010 2020
Top Down - Sequential
Bottom Up - Non-sequential
Gradual change in nanofabrication domain
Technological Uncertainty
3rd Gen. 4th Gen. to 5th Gen.
(NanoSystem) (Molecular Nanosystem/NBIC)
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DSA
Ribosome Protein: 5~50nm Cell: 10~30μm
Tissue: μm~cm Organ (Heart): cm
Process to Build Human Being
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What can we substitute CMOS for ? Source: Modified from C. Michael Garner, Sept.16, 2003, Intel
Alternative state variables
Spin, nuclear, photon
exciton
Phase; Multiferroics
Plasmonics
Quantum state
Magnetic flux quanta
Mechanical deformation
Dipole orientation
Molecular state
Required characteristics
Scalability : density/cost
Improved performance
Power efficiency
Gain
Operational reliability
Room temp. operation
Less than 10nm channel
Preferred approach
CMOS process
compatibility
CMOS architectural
compatibility
Up to now or maybe forever, no alternative variables can compete with electron.
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Variable Switching
Energy
Physical
Size Limit
Practical
Size Limit
Electron 2~4 KT 1nm
3-5nm
Spin
500 KT
7nm
>40nm
Photon 3600 KT 20nm
>90nm
Switching energy: from 0 state to 1 state
Spin & Photon are not alternative for Electron as a switching device due to the power consumption
The infrastructure for spin and photon would require a considerable change from what the industry is doing today.
Physical & Practical Limits of State Variables Source: J.A. Hutchby et al., in ICSICT, October, 2006 , Shanghai, China p1049
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Proposed Emerging Memories for Tera-level
CMOS Based Memory (Evolutionary) - FRAM - MRAM (Magnetic RAM) - PRAM (Phase Change RAM) - FBDRAM (Floating Body DRAM) - NFGM (Nano Floating Gate Memory) - MONOS (Metal Oxide Nitride Oxide Semiconductor) - PoRAM (Polymer RAM ) - RRAM (Resistive RAM) Beyond CMOS Memory (Revolutionary)
- Single Electron Memory - Tracked MRAM - MoRAM (Molecular RAM) - CNT Memory - CBRAM (Conductive Bridge) - Cross-bar (CNT, Resistive, Magnetic) - NEMS Memory: Very high voltage (100 volt) - Memristor
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Risk Factors for the Future NVM Source: Modified from EE Times, April 4, 2011 after M. Durcan, Feb., 2011
NAND PRAM CBRAM RRAM STT-MRAM
MRAM FRAM Molecul
ar
Data Retention
Medium Low Medium Extreme
Low
Low
Low
Extreme
Bit Density
Low Extreme Medium Medium Extreme Extreme Extreme High
Endurance Medium Low (?)
Low (?)
Extreme
Low
Low
Low
Extreme
Power per Bit
Low High Low Low High Extreme High High
Manufactu-rability
Medium Medium Extreme Medium Extreme Extreme Extreme
Extreme
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Generic Road-blocks to Tera-level Memory
CMOS-based Conventional/Evolutionary Memory: the same
as the CMOS road-block to scaling–down
- Lithography: EUV, Imprint, E-beam, Bottom-up
Not ready for above 256 Giga Flash
EUV: End of the road
- Device: SCE, Leakage, Read/Write Disturbance
- Reliability: Retention, Endurance
- Not scalable to tera-level unless 3-D integration is applied
Emerging Memory (revolutionary)
- Uncertain for feasibility as a device (cell level demonstration o.k.)
- Uncertain for reliability, reproducibility and manufacturability
What is graphene good for?
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Electronics:
- High frequency devices utilizing the highest mobility ever
(200,000cm2/Vs at RT: 1,400 for Si and 8500 cm2/Vs for GaAs)
- Interconnet utilizing high current capacity (108 A/cm2) and
lower resistance (1μΩ-cm: 35% less than Cu)
- Heat pad using high thermal conductivity (5 KW/mK: 10 x larger than
Cu and Al)
Transparent Electrode: by seeding plastics with just 1%
- Replacement of ITO (Transparency; 90%, Resistance: 30 Ohm/sq)
Spintronics:
- Potential high spin injection efficiency due to the larger spin diffusion
Mechanical:
- Composite Matls. (Young’s Modulus: 1.0 TPa, Intrinsic Strength: 130 GPa)
Chemical:
- Highest surface to volume ratio ever if utilizing two-side surfaces
Energy Storage:
- A super-conductive membrane between the battery’s poles leading to
ultra-capacitors
Graphene was originally seen as a material that could replace Si in
digital logic circuits. Grahene does not have a bandgap, and its
transistor is very difficult to turn off (on/off ratio= <~1,000).
- Opening a gap of just 1eV is necessary to make graphene ribbons
smaller than 2 nm with single atom precision
Is it possible using current fabrication technology?
- For bilayer graphene, creating a gap of 0.25eV requires around
100 V and you would simply not have access to such high voltages
in devices like cell phones, laptops or tablets
The CVD graphene is not a single crystal and can not be. This leads to
serious problems in the application of nanoelectronics-logic and memory.
- Mobility degradation and variation in properties
- No advantage over other single crystalline high mobility semicond.(Ⅲ-Ⅴ)
It's becoming clear that graphene's promise is not in electronics,
but lies elsewhere. Challenges not the same as those by CNT
- CNT challenges: impossible a few years ago and still impossible now
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What is graphene bad for?
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Graphene Synthesis and Applications
Catalog no. K12864, October 2011 c. 370 pp., ISBN: 978-1-4398-6187-5 $129.95 / £82.00
Edited by Wonbong Choi: Florida International University
Jo-Won Lee: Hanyang University
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What have we achieved for superintelligent nanosystem through TND for last 10 years?
●W
Ls
●B
L
s ●SSL ●GS
L
●PI
PE
NAND Flash (3D + CTF): VLSI 2009
Microphotograph of RTD 29GHz
VCO: 1/170 power consumption
AlGaSb: 1m
Si (001)
GaSb
AlSb
III-V Epi. Growth on Si
InSb QDs
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An all-Si single electrons at R.T. for ultra low-power computing
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Neutral Beam and Atomic Layer Etching Equipment & Processes
<35 nm Etch Pattern>
50nm
35nm
35nm Si pattern etch • The charging damage could be removed by using neutral beam instead of inductively coupled plasma.
• Highly anisotropic etch profile could be obtained.
• Significant property improvement of InP HEMTs device by atomic layer etching without damaging (gate recess)
1E9 1E10 1E11 1E12 0
10
20
30
40
50
ALET RIE
f T =100 GHz
Frequency [ GHz ]
f T =166 GHz
L g =0.3 m, Wg =20 m
H 2
1 [
dB
]
Un
it c
urr
en
t g
ain
,
Lg=0.25 m
<InP HEMTs Device Characteristics>
I G (
A)
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Epi. Graphene by Thermal Decomposition of SiC
Thermal decomposition of SiC wafer surface under vacuum
of 10-6 to 10-5 torr
1300 to 1500oC growth regime
Growth phenomena on silicon and carbon faces
- Si face : 1~ 2 layers, uniform
- C face : 2~5 layers, thicker graphene, high mobility
Raman peaks of graphene on C-face - D peak (1,350) defect,
- 2D peak (2,700) - G peak (1,620) graphene
0.00E+00
2.00E-04
4.00E-04
6.00E-04
8.00E-04
-10 -5 0 5 10
Graphene Transistor: W x L(50um x 50um)
0.5V
1V
Vg (V)
Id (A)
Field Effect mobility: 980 cm2/Vs
TEM
RAMAN
1,500 3,000
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Metal gate
GST
ALD SiO2
Thermal SiO2
p- Si Substrate
Non-annealed Sample:
T↑ → R↓ ⇒ Meta-stable
FCC Crystalline Phase
H2 Annealed Sample:
T↑ → R↑ ⇒ Stable HCP
Crystalline Phase
New Single Element Memory using GST
5um*5um
-1 0 1 2 3 4 10f
1p
100p
10n
1
100
1m
Dra
in C
urr
en
t, I
D,(
A)
Gate Voltage, VG,(V)
No Anneal @ VD = 0.1V No Anneal @ VD = 2.0V Anneal @ VD = 0.1V Anneal @ VD = 2.0V
Temperature, T('C) 0 20 60 100 140 180
100
1k
10k
100k
1M
125?
1.25m
12.5m
125m
1.25
Resis
tivit
y,
ρ(Ω
*cm
)
Resis
tan
ce,
R [
Oh
m]
Heat Up @HB Test Cool Down @HB Test H2 Anneal @Full F/O No Anneal @Full F/O
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Thank you!