development of core technologies for green nanoelectronics · fujitsu laboratories ltd. (core...
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Naoki Yokoyama Leader, Green Nanoelectronics Center, AIST
Fellow, Fujitsu Laboratories Ltd. (Core Researcher, FIRST Program)
Development of Core Technologies for Green Nanoelectronics
November 3, 2011
2nd Berkeley Symposium on Energy Efficient Electronic Systems
Acknowledgements: This research was funded by JSPS through the Funding Program for World-Leading Innovative R&D on Science and Technology (FIRST Program), initiated by the Council for Science and Technology Policy (CSTP).
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Acknowledgements Development & application of nanocarbon materials
“Synthesis and transistor application of graphene” Shintaro Sato, Group Leader Fujitsu
Mizuhisa Nihei, Group Leader Fujitsu
Toshimichi Shintani, Subtheme Leader Hitachi
Junji Tominaga, Group Leader AIST
“CNT/graphene interconnects”
“Development of low power superlattice phase-change material and its processing technology for device”
Material research for backend devices
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Under One Roof
nano
June 17, 2009 President, University of Tsukuba Nobuhiro Yamada President, National Institute for Material Science (NIMS) Teruo Kishi President, National Institute of Advanced Industrial Science and Technology (AIST) Tamotsu Nomakuchi Chair, Committee on Industrial Technology of Nippon Keidanren Ryoji Chubachi
Tsukuba Innovation Arena for Nanotech
TIA Nano Univ. of Tsukba
NIMS
AIST
By adopting joint strategies and management for R&D and education to contribute to the growth of the Japanese and global economies.
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Univ. of Tsukuba
AIST
Central R&D Hub for Nanotechnology
Core Competencies of TIA Nano Started April 2010
Nano-Material SafetyIntegrative data center and research frame
for nano-material safety
Power ElectronicsIntegrated R&D frame from SiC wafer,
device to power system
N-MEMS
High-value-added niche MEMS and mass production integrated N-MEMS
Carbon NanotubesR&D framework of CNT mass production and CNT composites for wide applications
Nano-GreenR&D framework for green innovation
driven by nanotechnology
Nanoelectronics・Backend device・New material・Advanced lithography(EUVL)
Nanodevice Research Foundry・Prototype device(45-65nm CMOS and N-MEMS,etc.) fabrication and evaluation(φ200-300mm)・SiC power device fabrication and evaluation
Nanotech Open User Facilities
Open user research facilities in AIST and NIMS (nanocharacterization, nanoprocessing,etc.)
Networking School of Nanotechnology
Graduate school function through cooperation of University of Tsukuba and partnering universities
6 Core Research Domains
3 Core Infra-
structures
・Nano CMOS・Silicon-photonics・Carbon-electronics・Spintronics
4500 m2 super-clean room
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Enterprise companies
Enterprise companies
Vice President, AIST
Nanoelectronics Research Institute
FIRST: N. Yokoyama Development of core
technologies for green nanoelectronics
SCR Driving Management team
4500m2
Super-clean room (SCR)
FIRST: Y. Arakawa Photonic-electronic integration system
METI: N. Sumihiro
Super-low-voltage devices for low-carbon society
FIRST: H. Ohno Ultralow-power spintronics-
based logic VLSIs
Partial funding
Nanoelectronics Consortium
TIA Promotion Division
Seven universities Two institutes
Researchers
30 researchers
METI: Ministry of Economy, Trade and Industry
Nanoelectronics R&D in TIA nano
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20 researchers
Renesas, ULVAC, Fujitsu, Toshiba, Hitachi
Background and R&D plans of Green Nanoelectronics Project Graphene growth and top-down
fabrication of graphene nanoribbons Latest hot news about interfacial phase-
change memory devices
Overview
(GMR > 2000% at 400 K)
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Paradigm Shifts in ICT Society
Broadband
Wireless
Broadband LAN
WAN
PAN
Public space
Personal space
Office
Home
BAN
Network centric
For everyone: Information search
Human centric, Ubiquitous
For anyone: Knowledge integration
Data center
Computer centric
For professionals: Data processing
Personal security/safety and social activities will be provided to everyone, resulting in a truly ubiquitous society.
7 Source: Fujitsu website
Future ICT will need to meet people’s requirements more precisely and become more user friendly and reliable.
190 times increase in traffic · 5.2 times higher · 20% of domestic electric power generation
Increased Power Consumption of ICT Source: Ministry of Economy, Trade and Industry, Japan For Japan
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2006 20250
50
100
150
200
Inte
rnet
traf
fic
Index (2006 = 1)
Year
637 Gbps
121 Tbps
A paradigm shift in ICT society could result in environmental destruction. Innovations are needed to develop an environmentally friendly ICT society.
0
5E+13
1E+14
2E+14
2E+14
3E+14
3E+14
2006 2025(Year)
Pow
er c
onsu
mpt
ion
(W
h)
Network devices
Display
Server/ Storage
13 times
5.2 times
2.5 times
~240 billion kWh
計算機室内の次世代スパコン (イメージ) “K” Designed by Japan’s RIKEN Research Institute and Fujitsu
800 racks of computing gear housing 80,000 Fujitsu SPARC 64 VIIIfx processors running at 2.2 GHz
The processors are interconnected with a high-capacity direct connection network that enables fast communication between neighbors.
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・No.1 in the latest Top500 supercomputers list ・Most energy-efficient systems in the list This system is now fully installed and it will be fully operational in 2012.
10-Petaflop K Supercomputer
Copyright 2010 FUJITSU LIMITED
SPARC64TM V (1 core) SPARC64TM VI (2 cores x 2 VMT) SPARC64TM VII (4 cores x 2 SMT)
SPARC64TM VIIIfx (8 cores) ・Large-instruction-set architecture ・Highly integrated systems on chip ・Water cooling for high reliability
ピーク性能と消費電力の推移
0
5
10
15
20
25
V V + VI VII VIIIfx
SPARC64
SPA
RC
64 V
= 1
.0
Power (W) = x 0.5
Performance (GF) = x 3
Peak performance vs power
To reduce the power consumption by another order of magnitude, we need to reduce the supply voltage to a half or less of its current value.
90 nm
65 nm
45 nm
130 nm 90 nm
2.2 Gflops/W: 128 Gflops@58 W
Supply voltage remained constant at 1.0 V for all processors in the SPARC64 series.
.
Progress of SPARC64
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Overview
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Background and R&D plans of Green Nanoelectronics Project Graphene growth and top-down
fabrication of graphene nanoribbons Latest hot news about interfacial phase-
change memory devices
(GMR > 2000% at 400 K)
Multilayer Graphene with Fe Catalyst
32 nm
Fe 20 nm
7 nm
20 nm
Graphene Graphene
10 nm Bilayer graphene
Source gas: C2H2/Ar Temperature: 650ºC Total pressure: 1 kPa Partial pressure of C2H2: 0.002−5 Pa Growth time: 1−20 min Catalyst: Fe film (100−500 nm)
Th
ickn
ess (n
m)
Pressure × Time (Pa·min)
Appears to be proportional to (Pressure × Time)1/2
Substrate
Graphene Fe film
Catalyst thickness: 200 nm
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D. Kondo, S. Sato, et al., Appl. Phys. Express 3, 025102 (2010).
We are using thermal CVD to grow graphene films using Fe catalyst film.
Pressure x Time
Thic
knes
s (n
m)
Subjects: ・Improvement of quality of graphene ・Connection of graphene & CNTs
Graphene Grown on a 200-mm Wafer
A B
C
D
E
Source gas: C2H4 Temp: ~860ºC
10 nm Cu film
TEM image
D G
2D
Graphene
200-mm wafer
Monolayer graphene
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Sato et al., ECS Trans. 35(3), 219 (2011) Sato et al., ECS Trans. 37(1), 121 (2011)
Graphene Tr for BPSK Modulator
R = 3 kW
Vdata
Vdata
Vsin Vsin
Vout
Vout
N. Harada et al., APL 96, 012102 (2010)
Vg (V)
0.03
0.08
0.13
0.18
-40 -20 0 20 40
I d(m
A)
W = 2.6 μmL = 8.5 μmVd = 1 V
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(Mechanical exfoliation)
n-type p-type
(Binary digital data)
(Sinusoidal carrier wave))
BPSK: Binary Phase Shift Keying
Phase modulation concept are widely used as a modern standard in digital wireless communication systems such as mobile phones and DTV broadcasting.
Two approaches for GNR fabrication
Bilayer graphene Graphene nanoribbon (GNR)
Zigzag type Armchair type
Bottom-up: ・ Self-organization of GNRs by preferential growth on high-index surfaces of Cu ・Chemical synthesis of GNRs (in collaboration with universities) Top-down: Lithography + etching (RIE)
Two Main Techniques for Band Gap Generation
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He ions Electrons
5 nm
Helium Ion Microscope in Fabrication of GNR
High-precision etching is possible because
No contamination from resist process because
He ion beam etching is ideal for GNR fabrication. However, on/off operation of current has not been realized yet.
smaller beam size than electron beam • de Broglie wavelength is 1/100 that of electron
direct etching of graphene without resist mask • free from edge roughness due to resist mask
5-nm-wide GNR fabricated by HeIM (image from Carl Zeiss website) 50 nm
Advantages:
direct etching of graphene
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Device Fabrication
5 nm
200 nm
SiO2 Sub. Graphene
S
D
50 nm
10 µm
1. Exfoliation of Single-Layer Graphene HOPG (GE; YZA grade) and “Scotch tape” 300-nm-thick SiO2 layer on Si substrate
2. S/D Contacts Ti/Au (5/30 nm) by Thermal Evap. + Lift-off Two-terminal resistance
3. GNR Fabrication Direct etching by He ion beam
0
1000
2000
3000
4000
5000
-30 -20 -10 0 10 20 30
R2t
(Ω)
1000
2000
4000
3000
0 0 30 −30
EF EF
VBG (V)
5000
(processed on March 10th)
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S. Nakaharai, et al., SSDM2011, p. 1300 (2011)
Graphene
GNR
0.0E+00
2.0E-12
4.0E-12
6.0E-12
8.0E-12
1.0E-11
1.2E-11
1.4E-11
-40 -20 0 20 40
VBG (V)
Vd = 1 mV T = 45 K
ΔVBG
ΔVBG ∼ 10 V Transport gap ∼ 200 meV
On/Off Operation by Back Gate Bias
VBG (V)
I d (A
)
1.E-14
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
-40 -20 0 20 400 40 20 −20 −40
10−7
10−8
10−9
10−10
10−11
10−12
10−13
10−14
1 mV
20 mV
100 mV
200 mV Vd=
0 40 20 −20 −40 0
2
10
4
6
8
12
14
I d (p
A)
T = 45 K
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S. Nakaharai, et al., SSDM2011, p. 1300 (2011)
Eg(eV)= 0.8/w(nm) Hongjie Dai's lab at Stanford University
Xiaolin Li, et al.,Science 319, 1229 (2008)
Overview
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Background and R&D plans of Green Nanoelectronics Project Graphene growth and top-down
fabrication of graphene nanoribbons Latest hot news about interfacial phase-
change memory devices
(GMR > 2000% at 400 K)
(3) New Materials for Back-End Devices PCRAM: Phase-change random access memory
• Conventional (GeSbTe) alloy materials: Structural changes between disordered and crystalline states
• Superlattice (GeTe/Sb2Te3) materials: Only Ge atoms move at the interfaces.
→ power consumption reduced by 1/10–1/100
Sb2Te3
GeTe
GeTe
Sb2Te3
low resistivity high resistivity
voltage pulse
Superlattice PCM is now referred to as interfacial phase change memory (iPCM).
Tominaga et al., Nature Nanotech vol. 6, 501−505 August 2011
Tetrahedrally bonded Ge atoms Octahedrally bonded Ge atoms
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Since Ge–Sb–Te alloys do not have a magnetic moment, magnetism was not thought to play a role in its switching dynamics or electrical properties.
Demonstration of Low Power Phase Change
0 Current (mA)
5 10 15 102
103
104
105
106
107
108 R
ead
resi
stan
ce (Ω
)
102
103
104
105
106
107
108
Rea
d re
sist
ance
(Ω)
Current (mA) 0 2 4 6
Conventional (Ge2Sb2Te5) iPCM (GeTe/Sb2Te3)
reset reset
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Applying a magnetic field to iPCM might affect the material properties, since Sb2Te3 was reported to be a topological insulator. This is because an in-plane external magnetic field is expected to further contribute to the splitting in spin states induced by the Rashba effect at the GeTe/Sb2Te3 interfaces.
Power reduction by 1/10
Tominaga
Nanoelectronics Research Institute National Institute of Advanced Industrial Science and Technology
E¥PCOS 2011, Switzerland Topological insulating state in interfacial phase-change memory
Comparison of the Switching Behavior
Ge1Sb4Te7 alloy iPCM [(GeTe)2(Sb2Te3)4]8
V (volt) V (volt)
I (m
A)
I (m
A)
Vset Vset Vset (mag.)
iPCM device Alloy device
Tominaga et al., Appl. Phys. Lett. 99, 152105 (2011)
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Blue lines: I-V curves under 0.1 T magnetic field in plane Black and red lines: I-V curves w/o magnetic field (before and after applying 0.1 T, respectively)
Vset: 0.85 V Vset: 2.0 V Vset: 0.85 V
ΔR/R =2000%
This finding paves the way for development of conceptually new memory devices that combine the merits of both phase-change and magnetic data storage.
Since our objective and R&D plans for green nanoelectronics seem to be quite similar to those of the Energy Efficient Electronic System Program, I anticipate there will be greater information exchange between them so that we can accelerate our research together to realize energy saving and human-centric ICT societies.
Thank you very much for your attention. 27