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8/13/2019 Adv CMOS Jongholee
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Semiconductor Materialsand Device Laboratory
Jong-Ho Lee
School of EECS and ISRC, Seoul National University
Bulk FinFETs: Fundamentals,
Modeling, and Application
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1
Introduction
Fundamentals of Bulk FinFETs
Modeling
Applications
Conclusions
Outline
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The scaling of conventional planar MOSFETs has been facing
problems such as subthreshold swing degradation, significant
DIBL, fluctuation of device characteristics, and leakage.
To solve the problems, 3-D device structures could be a solution
and have been studied.
FinFETs (built on bulk silicon or SOI wafers) among 3-D devices
are very promising candidate for future nano-scale CMOS
technology and high-density memory application.
For the bulk FinFETs which is going to be applied to mass
production, we discuss about fundamental properties, modeling,
and application of the bulk FinFETs.
Introduction
2
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Whats bulk FinFET?
FinFET
SOI FinFET Bulk FinFET
3-D view ofbulk FinFET
Si Sub
SiO2
G fin
Si Sub
SiO2
G fin
Low wafer cost
Low defect density
No floating body effect
High heat transfer rate
to substrate
Good process compatibility
S/D
S/D
Hin xj
WinTOX
Heat
Korea/USA patent
Bulk FinFETs (Double- or Tri-gate MOSFETs)
ID-VGS Characteristics of 40 nm bulk N FinFET
3
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S/D
S/D
H in xj
W inT OX
Heat
Comparison between Our Structure and Intels
Our Structure Intels StructureConventionalPlanar Structure
4
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5
As+, 20 keV 3x1015/cm2, 2 Fin
25 nm
50 nm
40 nm
-0.5 0.0 0.5 1.0 1.510-10
10-9
10-8
10-7 VDS = 0.1 V
Vbs = 0 V
Vbs = -1 V
Vbs = -2 V
DrainC
urrent(A)
Gate Voltage (V)
ID-VGS Characteristics of 40 nm bulk N FinFETOxide
Si
CMP and
partial etch-back
Poly-Si
40 nm
Gate Poly-Si Etching
T. Park et al., SNU/KNU, Physica E19, p.6, 2003T. Park et al., SNU/KNU, Nanomes03 2003
Top Si Width 25 nm
Bottom Si Width 100 nm
Si Fin Height 230 nm
First Bulk FinFET in the World
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T. Park et al., SNU/Samsung/KNU, p.135, Symp. on VLSI Tech. 2003
-0 .5 0.0 0.5 1.0 1.5 2.010
-14
10-13
10 -12
10-11
10-10
10-9
10-8
10-7
10-6
10-5
Conv. DRA M C el l Tr .DIBL = 108 m V/V
Vds = 0.1 V
Vds = 0.6 V
Vds = 1.1 V
Vds = 1.6 V
Dra
inCurrent(A
)
G ate Vol tage (V)
Vbs = 0 V
FinFET
DIBL = 24 mV /V
Fin Top W idth = 30 nm
Fin Bottom Width = 61 nm
Fin Height = 99 nm
LD R A W N
= 120 nm
W = 120 nm
L = 120 nm
181 nm
99 nm
61 nm
30 nm
82
Si Substrate
SiO2
Poly-Sifin body
SEM cross-section
Gate
Electr
ode
SiO2
SiN
SiSubs
trate
Fin
SiO2
6
First Bulk FinFET at Industry
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7
Introduction
Fundamentals of Bulk FinFETs
Modeling
Applications
Conclusions
Outline
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Gate
Oxide
Fin
Gate
Fin
Gate
Fin
(a) (b) (c)
DG Structure TG Structure
90o Corner Half-circle Corner
8
Body Shape of FinFET
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10 20 30 40 500.1
0.2
0.3
0.4
0.5
Nb=1x10
19cm
-3
Tox
=1.5 nm
xj,S/D
=66 nm
Hfin
=70 nm
Bulk
SOI
Fin Width (nm)
V
th
(V)
Lg
=25 nm
0
30
60
90
120
150
180
DIBL(mV/0.9V)
10 20 30 40 50
70
75
80
85
90
95
100
xj,S/D
=66 nm
Hfin
=70 nm
Nb=1x10
19cm
-3
Tox
=1.5 nmLg=25 nm
VDS
=0.9 V
Subthreshold
Swing(mV/dec)
Fin Width (nm)
BulkSOIVDS
=0.05 V
The bulk FinFETs (solid circles) have nearly the same Vth, DIBL, and SS
characteristics as those of SOI FinFETs (open circles).
Vth & DIBL SS
9
Equivalent FinFET on Bulk and SOI Wafers
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Equivalent FinFET on Bulk and SOI Wafers
Tri-gate on bulk-silicon and SOI substrates have similar short channel
performance
Source: Intel
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Heat transfer rate : Bulk SOI
Bulk FinFET has a device temperature less by 130 oC than SOI FinFET at a
fixed VGS of 0.9 V.
-0.2 0.0 0.2 0.4 0.6 0.8 1.0
300
325
350
375
400
425
450
475
130oC
Bulk
SOI
VDS=0.9 V
Tox
=1.5 nm
DeviceTemperature
(K)
Gate Voltage (V)
Lg=30 nm
12
Device Temperature Characteristics
Si Nanoelectronics, 102-103, 2003
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-1.00 -0.75 -0.50 -0.25 0.00 0.25 0.50
0.0
0.1
0.2
0.3
0.4
0.5
WFin
: 10, 15, 20, 30, 50 nm
WFin: 10, 15, 20, 30, 50 nm
Body Bias (V)
VT
(V)
70
80
90
100
110
120
Subthresh
oldSwing(m
V/dec)
LG=25 nm
No VT increase ata given back bias
S B
G G
Silicon Nanoelectronics workshop, p.102, 2003
Back-bias Effect
Properties of Bulk FinFETs13
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80 82 84 86 88 90 9280
90
100
110
120
LG=30 nm
HFin=70 nm WFin =20 nm
Angle () (deg)
DIBL(mV/V)
Na=1x10
19cm
-3
n+
poly gate
70
80
90
100
110
120
SS(mV)
20 nm
Fin
-0.2 0.0 0.2 0.4 0.6 0.8 1.00.6
0.7
0.8
0.9
1.0
1.1
1.2
VDS
=0.9 V
VDS=0.05 V
WFin
=20nm
HFin
=70nm
LG
=30nm
90o
83.3o
81.6o
Gate Bias (V)
N
ormalizedDrain
Current
Device Characteristics with Body Angle
Tapered fin widens degradedSCEs
Closer to 90o of body angle, better
DIBL and drain current
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Impact of Fin Profile
Rectangular Fin profile improves SCEs for LG scaling:
Lowers SSATLowers DIBL
Symp. on VLSI Tech, Intel, 2006
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Gate
Fin
Si Substrate
Gate
Fin
BOX
(a) (b) (c) (d)
Bulk SOI
Gate
Fin
BOX
Gate
Fin
BOX
Process variation
17
Bottom Corner Effect
Invited talk at ECS, ECSTransactions, 19 (4) 101-112 (2009)
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Ioff : (a) < (b) < (c) < (d)
-0.2 0.0 0.2 0.4 0.6 0.8 1.010
-11
10-10
10-9
10-8
10-7
10-6
10-5
10-4
Hfin
=70 nm
VDS
=0.05 V
VDS
=0.9 V
n+poly gate T
ox=1.5 nm
Wfin
=20 nm
Lg=100 nm
Bulk FinFET (a)
SOI FinFET (b)
SOI FinFET (d)
ID(A)
VGS
(V)
Nb=2x10
18cm
-3
(a) (b) (c) (d)0.01
0.02
0.03
0.04
0.05
0.06
SOI
Thresho
ldVoltage(V)
Bulk
Vth : (a) > (b) > (c) > (d)
ID vs VGS Vth vs Structure
18
Bottom Corner Effect
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Wfin DIBL & Vth
Low doped bulk or SOI FinFETs narrow Wfin for good characteristics
5 10 15 200.30
0.32
0.34
0.36
0.38
0.40
Simulation
Model
Fin Width (nm)
Vth
(V)
Hfin=70 nm
Lg=30 nm
Nb=5X1016cm-3
m=4.71 V
0
50
100
150
200
250
300
350
body
Si substrate
WFin
GateTOX
oxide
Local doping @ xP=80 nm
DIBL(mV/V
)
Rounded corner
corner effect
Low doped channel
Nb=5x1016 cm-3
Local doping
xp=80 nm
NLocal=3x1018 cm-3
19
Fin Body Width Effect of Bulk FinFET with Low Nb
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Planar MOSFET : Delay Time (due to Vth) with negatively increasing VBS
SOI or Bulk FinFETs : nearly constant Delay Time with VBS more
effective devices for the full-down circuits
-0.50 -0.25 0.00 0.25
0.8
1.0
1.2
1.4
1.6
Planar MOSFETBulk FinFET
SOI FinFET
Norma
lizedDelayTim
e
VBS(V)
Nb=2x10
18cm
-3C=20 fF
Tox
=1.5 nm Lg=50 nm
-0.50 -0.25 0.00 0.25
0.8
1.0
1.2
1.4
1.6
V1
CVb
Vcc
Vin
Full-down delay time vs VBS Inverter circuit
Speed Characteristics
ECS meeting (invited talk), May, 2008
20
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(a) Small signal equivalent circuit for RF device modeling.
(b) Comparison of RF parameters extracted from bulk and SOI DG FinFETs.
CgdRg
vgs
Gate
Drain
Substrate
gmvgsCm dt
dVgsCgs
gmbvbs
gds Csd
vbs
CjdCjs
Rsub
Source
P
O
R
T
1
P
O
R
T
2
Intrinsic Body
CgdRg
vgs
Gate
Drain
Substrate
gmvgsCm dt
dVgsCm dt
dVgsCgs
gmbvbs
gds Csd
vbs
CjdCjs
Rsub
Source
P
O
R
T
1
P
O
R
T
2
Intrinsic Body
177 GHz170 GHzfT
-0.0033 fF-0.0037 fFCsd
-fF0.0151 fFCjs
-8200 Rsub
-fF0.014 fFCjd
472 461 Rg
0.038 fF0.037 fFCgd
0.073 fF0.0713 fFCdg
0.113 fF0.116 fFCgs
0.414 S0.427 Sgds
166 S160 Sgm
0.286 V0.31 VVth
SOI DG
FinFET
Bulk DG
FinFET
177 GHz170 GHzfT
-0.0033 fF-0.0037 fFCsd
-fF0.0151 fFCjs
-8200 Rsub
-fF0.014 fFCjd
472 461 Rg
0.038 fF0.037 fFCgd
0.073 fF0.0713 fFCdg
0.113 fF0.116 fFCgs
0.414 S0.427 Sgds
166 S160 Sgm
0.286 V0.31 VVth
SOI DG
FinFET
Bulk DG
FinFET
(a) (b)
21
Speed Characteristics
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20 30 40 50 60 700.1
0.2
0.3
0.4
0.5L
g=100 nm
Tox
=1.5 nm
VGS
=1.0 V, VDS
=1.5 V
Na=3x10
18cm
-3
c=1x10
-7cm
2
n+poly gate
Solid : d=100 nm
Open : d=5 nm
Fin Width (nm)
Vdrop
(V)
2000
2200
2400
2600
2800
3000
3200 PeakElectronTempe
rature(K)
Effect of S/D Resistance with Fin Body Width
Wfin electron temp.
: Ohmic drop across Rsd (Wfin less than 50 nm)
Rsd=Ras+Rsh+Rc
22
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25
Introduction
Fundamentals of Bulk FinFETs
Modeling
Applications
Conclusions
Outline
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2-D schematic view of symmetric
double-gate MOSFET.
Gate
Gate
Source
(n+)
Drain
(n+)Fin
Body
Lov
Tox
Wfin
L
Lg
VGS
VGS
VDS
Oxide
y
x
0
Bulk FinFET or SOIFinFET (not shown)
Side-channel
S/D
S/D
TFOX
A
A
Side-channel of bulk or SOI FinFETs :
DG structure key point
26
Schematic View of DG MOSFETs
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27
Short-channel effect
xm xm
S D
xls xld
Lc=L-2xm
xrs=xcs xrd=xcd
S
(a) (b)
xcs
xhs
G
G
Tox
Wfin
SiO2
SiO2
b dep hs hd th ,SC E
ox c
qN x x x / 2V
C L
b dep
th ,SCE FB B
ox
h
c
qN xV V 2 1
C
x
L
Charge-sharing length
hs hd
h
x xx
2
: Vth model of the conventional
planar MOSFETs
:DG M OSFETsfin
0.5W
Vth Modeling of Side-Channel (1)
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28
Narrow-width effect
S DG
xhs xhdLg
Hg
Lc
xdf
(a) SiO2 SiO2Fin
Body
xdf
Hg G G
TgateTox
Wfin
(b)
b d e p d f
t h , N W E o x g
q N x x
V C 4 H
gateox
th ,s 2
dep b
d
ox
f
T8V ln 1
x qNx
T
: an effective widthdepleted by gate fringingfield
Vth Modeling of Side-Channel (2)
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Vth Modeling of Bulk FinFETs
g
M S B
E
2 e
b d e p d f t h , N W E
o x g
q N x xVC 4 H
gateox
of
ox
T2C ln 1
T
gateox
df th ,w oc 2
dep b ox
T8x V ln 1
x qN T
b dep df h
th ,w oc FB B w
ox m g
qN x xxV V 2 1
C L 2 x 4 H
b dep hs hd
th ,SCE
ox m
qN x x xV
C 2 L 2 x
Vth equations of bulk FinFETs based on 3-D charge sharing
SCE
NWE
: in NMOSFET with n+ poly gate
Thexdf and the
Vth,woc are
obtained by
solving theseequations
b dep h
th ,SC E FB B
ox m
qN x xV V 2 1
C L 2 x
IEEE Trans on Electron Devices, p. 537, 2007
29
30
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0.0 0.2 0.4 0.6 0.8 1.0
0.08
0.12
0.16
0.20
WB=15 nm
L=60 nm
gm,max
Method
Proposed Model
CC Method
L=30 nm
L=190 nm
Vth
(V)
VDS
(V)
Tox
=1.5 nm
Nb
=5x1018
cm-3
n+poly gate
Vth0
0.0 0.2 0.4 0.6 0.8
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
Simulation
Proposed Model
CC Method
ID(mA/m)
VDS
(V)
n=200 cm2
/V-sec n+
poly gateW
B=15 nm
Tox
=1.5 nm
VGS
=0.4 V
L=30 nm
Nb=2x10
18cm
-3
VDS,sat
=0.426 V
Nb=5x10
18cm
-3
VDS,sat
=0.271 V
Vth Model Considering Drain Bias
Jpn. Journal of Applied Physics
Verification in Double-Gate MOSFETs
30
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32
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0.0 0.2 0.4 0.6 0.8 1.010
-10
10-9
10
-8
10-7
10-6
10-5
10-4
10-3
VGS
(V)
ID(A/m)
Nb=5x10
18cm
-3
Wfin
=15 nm
Tox
=1.5 nm
VDS
=0.05 V
n=200 cm
2/V-sec
n+poly gate
0.0
0.2
0.4
0.6
0.8
1.0Simulation
Model
ID(mA/m)
Vth=0.1297 V
L=30 nm
L=190 nmV
th=0.1899 V
0.0 0.2 0.4 0.6 0.8
0
2
4
6
Simulation
Model
I
D,drift(mA/m)
VDS
(V)
Nb=5x10
18cm
-3
n+poly gateW
fin=15 nm
VGS
=0.4 V
Tox=1.5 nm
n=200 cm
2/V-sec
L=30 nm
VDS,sat
=0.274 V
VDS,sat
=0.679 V
VGS
=0.8 V
Nb=5x1018 cm-3, Wfin=15 nm, Tox=1.5 nm, n=200 cm
2V-1s-1
ID vs VGS ID vs VDS
Models show a good agreement with simulation data.
32
DC Models of Doped DG MOSFETs (3)
33
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33
oxide
Si substrate
Gate
Body
Wsc
Ws
WtcWtc
channel
Wsc
Ws
Hg
xh
bodyWfin
Gate
Tox
r
xdep
Wc
(a) (b) (c)(a) Schematic 3-D view for considering the
corner effect
(b) Cross-sectional view of the fin body
with 90 o corner
(c) Cross-sectional view of the fin body
with half-circle corner
Schematic Views for Considering Top Corner
Effect
33
34
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h2 x
13 L
,
' 0.5 2
2 13
c b fin hFB B
ox
th c
q N WV
CV
L
Vth,s model for side-channel with a fully depleted fin body
Vth,c model for corner-channel with a fully depleted fin body
: SCE term in the corner region regardless of the corner shape
: Corner Vth model
Corner factor(=0.4)
: Fitting parameterCorner-channel
b fin dfhF B B
ox g
th ,s
qN 0.5W xV 2 1
C L 4 H V
SCE & NWE
Side-channel
SCE NWE
bulk FinFET only
34
Vth Model of FinFET with Top Corner (1)
35
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20 30 40 50 60 70 80 90 100-0.2
0.0
0.2
0.4
0.6
0.8
1.0
c=0.4
VDS=0.05 V
n+poly gate
Nb=5x10
18cm
-3
MS
=-1.0683 V
W fin=20 nmH
fin=70 nm
Tox
=1.5 nm
Nb=10
19cm
-3
MS
=-1.0862 V
oxide
Si substrate
body
WFin
GateTOX
Si substrate
oxide
Simuation
Model
Vth
(V)
Gate Length (nm)
5 10 15 20
-0.1
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7Gate
Tox
body
Si substrate
oxide
Wfin Hg
c=0.4
Nb=5x10
18cm
-3
MS
=-1.0683 V
Nb=10
19cm
-3
MS
=-1.0862 V
Lg=100 nm
Simuation
Model
Vth
(V)
Wfin
(nm)
n+poly gate
Tox
=1.5 nm
VDS
=0.05 V
Hfin
=70 nm
Vth vs Lg Vth vs Wfin
Models show a good agreement with simulation data.
Hfin=70 nm, VDS=0.05 nm, Tox=1.5 nm, n+ poly gate
35
Vth Model of FinFET with Top Corner (3)
36
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Vth Modeling of Bulk FinFETs
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0Mod.
c=0.25
Lg=100 nm
m=4.71 V
m=4.17 V
10.60.3
Radius Ratio [=r/0.5Wfin]
r
0.5Wfin
Body
Nb=1x1019cm-3, H
g=70 nm
Nb=5x10
18cm
-3, H
g=70 nm
Nb=5x10
18cm
-3, H
g=40 nm
Nb=2x10
18cm
-3, H
g=70 nm
Vth
(V)
0
VDS
=0.05 VW
fin=20 nm
Sim.
30 40 50 60 70 80 90 100-0.2
0.0
0.2
0.4
0.6
0.8
1.0
c=0.25
VDS
=0.05 Vn
+
poly gate
Nb=5x10
18cm
-3
MS
=-1.0683 V
Wfin
=20 nm
Hg=70 nm
Tox
=1.5 nm
Nb=10
19cm
-3
MS=-1.0862 V
oxide
Si substrate
body
WFin
GateTOX
Si substrate
oxide
SimuationModel
Vth
(V)
Gate Length (nm)
Verification of the Model
IEEE Trans on Electron Devices, p. 537, 2007
36
37
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3-D schematic view 2-D schematic view
Bulk FinFET
as an example
S/D
S/D
Hg
XjSDE
0
WfinTFOX
A
A
body
Gate
Si substrate
oxide
Top-channelregion
Field
penetrationregion
from top-gate
Electricfield
The electric field penetration region
(hatched triangle) from the top-gate into
the side-channel region.
Current Model of FinFET (1)
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ID vs VGS
With Vth,s & Vth,c
Before considering field penetration
effect
With Vth0,s & Vth0,t
After considering field penetration
effect
-0.2 0.0 0.2 0.4 0.6 0.8 1.010
-14
10-13
10-12
10-1110
-10
10-9
10-8
10-7
10-6
10-5
10-4
Hg=70 nm
VDS
=0.05 V
Wfin
=20 nm
Lg=100 nm
Simulation
Side-channel (model)
Top-channel (model)
Total (model)
ID(A)
VGS(V)
Nb=5x10
18cm
-3
-0.2 0.0 0.2 0.4 0.6 0.8 1.0
0.0
1.0x10-5
2.0x10-5
3.0x10-5
Simulation
Side-channel (model)
Top-channel (model) Total (model)
ID(A)
Nb=5x10
18cm
-3
Lg=100 nm
Wfin
=20 nm
VDS
=0.05 V
Hg=70 nm
10-14
10-13
10-12
10-11
10-10
10-9
10-8
10-7
10-6
10-5
10-4
ID(A)
VGS
(V)
Current Model of FinFET (5): An Example
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ID vs VGS
Continuous Current Model of DG MOSFET
0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1
1.0x10-5
2.0x10-5
3.0x10-5
4.0x10-5
5.0x10-5
6.0x10-5
7.0x10-5
8.0x10-5
9.0x10-5
1.0x10-4
0.0 0.2 0.4 0.6 0.8 1.010
-14
10-13
10-12
10-11
10-10
10-9
10-8
10-7
10-6
10-5
10-4
Simulation
Nb= 2x10
18cm
-3
Nb= 10
18cm
-3
Nb= 10
17cm
-3
Nb= 0 cm
-3
ModelId(A)
Vgs
(V)
Vds
=1V
tox
= 1.5nm
tb= 10nm
Lg= 1m
W = 1m
Lines: Model
Symbols: Simulation
g=bg= midgap when Nb=0
No source/drain resistances
Good agreement
From intrinsic to ~1017 cm-3:
nearly the same
bsi
bb
t
x
q
kTtxqNx
2coslncosln
2
8
)4()(
22
.tan4
2
oxb
oxsi
ox
oxbbfbgs
qt
kTtttqNVV
.22/
0
)(
d
s
b
ft
kT
q
i
f
g
nd eqndL
WI
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Introduction
Fundamentals of Bulk FinFETs
Modeling
Applications
Conclusions
Outline
S f41
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First SRAM Application of Bulk FinFET
Bulk FinFETControl planar FET Nano width planar FET
Inverter
schematic
SNM Comparison
IEDM, p.27, 2003
SEM
Top
view
IEEE Trans on Electron Devices, p.481, 2006
B lk Fi FET i SRAM C ll42
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Si
SiO2
SiN
GatePoly
-Si
SiFin
-1.00 -0.75 -0.50 -0.25 0.00 0.25
10-10
10-9
10-8
10-7
10-6
10
-5
10-4
10-3
10-2
10-1
DrainCurre
nt(A)
Gate Voltage (V)
Triple Gate PMOSFET, Vds = -0.1 V
Triple Gate PMOSFET, Vds = -1.1 V
Planar PMOSFET, Vds = -0.1 V
Planar PMOSFET, Vds = -1.1 V
VBS
= 0 V
-2.5 -2.0 -1.5 -1.0 -0.5 0.0
0.0
-1.0x10-5
-2.0x10-5
-3.0x10-5
-4.0x10-5
-5.0x10-5
-6.0x10-5
-7.0x10-5
DrainCurre
nt(A)
Drain Voltage (V)
VBS
= 0 V
Solid : Triple Gate PMOSFET
Dashed : Planar PMOSFET
IEEE Electron Device Letters, p. 798, 2004
Bulk pFinFET in a SRAM Cell
SEM View and I-V Curves of pMOSFET
SEM view
ID-VGS curves
ID-VDS curves
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World 1stSaddle MOSFET for DRAM Cells
Si sub.
S/D
SiO2
Fin body
Gate A`
A
BB`
IEEE Electron Device Letters, p. 690, 2005
A A`
B B`
xjS /D
Gateinsulator
G
ate
S /D
L g
Gateinsulator
Gate
S iO 2
Si sub.
W fin
L ov_side
Localdoping
-0.3 0.0 0.3 0.6 0.9 1.2 1.510
-16
10-14
10-12
10-10
10-8
10-6
10-4
Saddle m 4.71 V
Recess m 4.17 V
VDS
=
0.05 V 1.5 V
Saddle
Recess
Drain
Current(A)
Gate Voltage (V)
Lg=12 nm W
fin=20 nm T
ox=3.5 nm
Recess depth=50 nm
xjS/D,LDD
=21 nm
xjS/D,HDD
=33 nm
Schematic View and Comparison of I-V Curves
Saddle Recess
SS 69.5 132
DIBL 21 170
Schematic view
Korea/USA patents
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Summary
Brief introduction
Fundamentals of Bulk FinFET
- Nearly the same scalability and performance as those of SOI
FinFET, and has several advantages
- Body shape, temperature, back-bias, S/D resistance, and speed- Design guideline on body doping and width
Model explains very well the behavior of Vth, internal physics, and
I-V of double/tri-gate bulk FinFETs
Bulk FinFETs could be applied to SRAM, low-power logics, and be
modified to DRAM cell