Post on 27-Feb-2020
14. November 2007 Theo Mustermann
Unsere Ziele Das Forschungszentrum Jülich im Fokus
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Strained Si Nanowire Tunnel FETs and
Inverters
Qing-Tai Zhao
Peter Grünberg Institut (PGI-9)
Forschungszentrum Jülich, 52425 Jülich, Germany
Peter Grünberg Institute (PGI-9) 2
Outline
• Introduction
• Scaled Strained Si NW TFETs and Inverters
• New structures and new materials for TFETs
• Summary
Peter Grünberg Institute (PGI-9) 3
STEEP SLOPE DEVICES: Tunnel FETs
Dynamic power dissipation
~ VDD2 . f
Static power dissipation
~ VDD . IT . exp (IT/S)
A. Ionescu, H. Riel
Nature 2011
For MOSFET with ideal SS,
60 mV of VDD decrease results in 10 x Ioff
Peter Grünberg Institute (PGI-9) 4
At equal standby power and switching
energy, TFET logic can operate with a ~8x
performance compared to MOSFET. U. E. Avci et al. (Intel), VLSI 2011
TFET vs MOSFET: Operation
Peter Grünberg Institute (PGI-9) 5
Band-to-Band Tunnel FET Challenges:
High on-currents
Steep slope for a large ID range
Ambipolar switching
Steep tunneling junctions
Trap assisted tunneling
Metal gate
TAT
TAT sets in at low VGS
BTBT
Vandooren et al. SSE 83,(2013)
Peter Grünberg Institute (PGI-9) 6
Eg , m*, band alignment in heterostructures
Si, strained Si, SiGe, … sGe, GeSn…..
Electrostatics: = dop + ch
dop : Tunnel-junctions: steep profiles, no defects
ch : Device layout : planar NW
Band to band tunneling
λ : Screening length of
electrical potential
Eg: Bandgap
m*: Effective mass
Reviews: J. Knoch et. al in „Nanoelectronics and IT“ ed. R. Waser, J. Wiley, (2012) p.341
A. Seabaugh & Q. Zhang, Proc. IEEE 2010 DOI:0.1109/JPROC.2010.2070470
Drain Drain
Source
Gate
Source
Gate
smaller Eg
)(3
24exp~
g
23
g
WKBEq
EmTIds
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Process to form p- and n-Tunnel FETs
Tilted ion implantation with TiN gate as shadow mask into the SILICIDE
sSi NW array
HfO2/TiN
Peter Grünberg Institute (PGI-9) 8
sSi NW array
HfO2/TiN
S/D silicidation
L. Knoll et al. ESSDERC 2012
Process to form p- and n-Tunnel FETs
Tilted ion implantation with TiN gate as shadow mask into the SILICIDE
Peter Grünberg Institute (PGI-9) 9
Process to form p- and n-Tunnel FETs
sSi NW array
HfO2/TiN
S/D silicidation
B+ implant at 135°
B+ implant
Tilted ion implantation with TiN gate as shadow mask into the SILICIDE
Peter Grünberg Institute (PGI-9) 10
Process to form p- and n-Tunnel FETs
sSi NW array
HfO2/TiN
S/D silicidation
B+ implant at 135°
As+ implant
As+ implant at 45°
Tilted ion implantation with TiN gate as shadow mask into the SILICIDE
Peter Grünberg Institute (PGI-9) 11
Process to form p- and n-Tunnel FETs
sSi NW array
HfO2/TiN
S/D silicidation
B+ implant at 135°
As+ implant at 45°
Out diffusion at 450°C
Tilted ion implantation with TiN gate as shadow mask into the SILICIDE
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0 5 10 15 2010
1
102
103
104
105
Coun
ts
Depth (nm)
Ni
As
1.4nm/dec
0 5 10 15 20 25 30 35 4010
0
101
102
103
104
105
Co
un
ts
depth (nm)
3.2nm/dec
500°C 1min
B+ implantationNiSi2
Steep junction formed by IIS
5keV As into NiSi2: 750°60s
Very steep junctions !
implant
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Doped silicide contact of sSOI NW TFETs
Advantages of IIS with NiSi2 • Steep junctions • Perfect gate alignment • Low S/D resistance • Less defects in Si (Less TAT)
Peter Grünberg Institute (PGI-9) 14
Complementary NW-array TFETs
L. Knoll et al. EDL34 (6) 813 (2013)
High Ion (VDS=0.5V):
10.3 µA/µm for the p-TFET
18.3 µA/µm for the n-TFET
Peter Grünberg Institute (PGI-9) 15
L. Knoll et al. EDL34 (6) 813 (2013)
SS (min)~30mV/dec
Ambipolar characteristics due to
symmetric doping.
Complementary NW-array TFETs
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Suppressed TAT by pulse measurements
More results will be presented in IEDM 2013
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First logic circuits:
Complementary NW-array TFET Inverter
L. Knoll et al. EDL34 (6) 813 (2013)
Peter Grünberg Institute (PGI-9) 18
First sSi-TFET-Inverters:
L. Knoll et al. EDL34 (6) 813 (2013)
Voltage transfer characteristics (VTC):
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First sSi-TFET-Inverters:
L. Knoll et al. EDL34 (6) 813 (2013)
Overshoot due to enhanced
Miller capacitance
S. Mookerjea et al. EDL 30 (2009)
-0.5
0.0
0.5
1.0
1.5
VIN
,VO
UT (
V)
0 25 50 75
VOUT
@VDD
=1V
Time (ns)
Inverter time response:
fall time ~2 ns;
Voltage transfer characteristics (VTC)
Peter Grünberg Institute (PGI-9) 20
10nm Si GAA NW-TFET
NW array
Lars Knoll Proc. ULIS conf. 2013
Optimized electrostatics by GAA
Higher current: 75µA/µm @VDS=1V
Smaller SS
suppressed ambipolarity due to
different doping at drain side
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Nanowires outperform planar devices !
T- dependence: planar vs NW Si TFETs
Steeper
Slopes
and less
TAT
with NWs
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Benchmarking: Si & Ge TFETs
11
11
VDD=1.0V
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10nm Si GAA NW-TFET
µA/µm
Nikonov et al. IEDM 2012
TARGET
Peter Grünberg Institute (PGI-9) 24
10nm Si GAA NW-TFET
µA/µm
Nikonov et al. IEDM 2012
TARGET
We need ~10 x more Ion
at Vdd = VG = 0.3 V !
High strain
New material: sGe, GeSn
Peter Grünberg Institute (PGI-9) 25
Implementation of local strain at source
Smaller Eg at source higher BTBT
Larger Eg at drain suppressed
ambipolarity
• Strain accumulation through
relaxed pads
• Si-NW tensile strained up to
4.5%
reduces 𝑬𝑮 to 0.5 eV
R.A. Minamisawa et al., Nature Communications, 2013
See Poster No. 9, by Lars Knoll et al.
Peter Grünberg Institute (PGI-9) 26
SiGeSn Tunnel FET
S. Wirths et al., Appl. Phys. Lett. 2013
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SiGeSn Tunnel FET
S. Wirths et al., Appl. Phys. Lett. 2013
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• Box-shaped doping profile
• ECV: B-doping ~ 1019 cm-3
• AFM: rms = 0.8 nm
SiGeSn Tunnel FET
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NW TFETs:
• Improved tunneling junction by IIS and DS
• Scaled NW diameter higher Ion (75µA/µm @ 1V)
less TAT, smaller SS
TFET inverters:
• High VTC gain
• Sharp Transition at VDD=0.2V
Future: highly strained Si NW structure
strained Ge …Si-Ge-Sn
…..may become competitive with III-V !
Conclusions
Peter Grünberg Institute (PGI-9) 30
Acknowledgements
Lars Knoll
Simon Richter
Stephan Wirths
Matthias Schmidt
Sebastian Bläser
Gia Vinh Luong
Anna Schäfer
Alexander Nichau
Andreas Tiedemann
Patric Bernardy
Dan Buca
Jürgen Schubert
Siegfried Mantl
sponsored by:
Peter Grünberg Institute 9
EPFL Adrian Ionescu (coord.)
IBM, RWTH Aachen, LETI, IUNET
Globalfoundries, Intel Mobile
Jülich
Helmholtz Nanofacility
K.Bourdelle