tunneling transistors for low power electronics
TRANSCRIPT
Tunneling
Transistors for Low
Power Electronics
James Teherani, Tao Yu,
Dimitri Antoniadis, Judy Hoyt
September 16, 2013
Support from
NSF E3S Center
MOSFET Scaling Crisis
September 16, 20133
Frequency scaling stalled
Power density of nuclear reactor
A. Danowitz, K. Kelley, J. Mao, J. P. Stevenson, and M. Horowitz, βCPU DB: Recording Microprocessor History,β Queue, vol. 10, no. 4, pp. 10:10β10:27, 4/2012.
1985 1990 1995 2000 2005 2010 2015
10 GHz
3 GHz
1 GHz
300 MHz
100 MHz
30 MHz
10 MHz
Pro
cesso
r C
lock S
pe
ed
September 16, 20134
Power & Voltage Scalingππππ‘ππ£π = πΌπΆπππ
2 π
ππππ π ππ£π = πΌππππππ + πΌπΊπππ
0
1
2
3
4
5
1970 1980 1990 2000 2010
Vdd
(Vo
lts)
Voltage scaling stalled
ππ‘ππ‘ππ = ππππ‘ππ£π + ππππ π ππ£π
A. Danowitz, K. Kelley, J. Mao, J. P. Stevenson, and M. Horowitz, βCPU DB: Recording Microprocessor History,β Queue, vol. 10, no. 4, pp. 10:10β10:27, 4/2012.
Transfer Characteristics
September 16, 20135
de
ca
de
mV
Dra
in C
urr
ent
(Ou
tpu
t)
Gate Voltage(Input)
πΌπππ
πππ2 πππ1
πΌππ2πΌππ1
Transistor
log(πΌ)
SSβsubthreshold swing (mV/decade)
Input
Output
p-type
DielectricGate
n-MOSFET
Input
Output
Sourcen-type
Drainn-type
Decrease SS
Transfer Characteristics
September 16, 20136
Dra
in C
urr
ent
(Ou
tpu
t)
Gate Voltage(Input)
πΌπππ
πππ2
πΌππ2
Transistor
log(πΌ)
SSβsubthreshold swing (mV/decade)
Input
Output
Increased πΌππfor small πππ
p-type
DielectricGate
n-MOSFET
Input
Output
Sourcen-type
Drainn-type
September 16, 20137
If:
Reduce SS (subthreshold swing)
Then:
β πππβ ππ‘ππ‘ππ
SSβSubthreshold Swing (MOSFET)
September 16, 20138
Ener
gy
n-MOSFET
x
Energy distribution of electrons
π πΈ = π(πΈ) β ππ·ππ(πΈ)thermal tail
CB
VB
Off-state current
π πΈ β1
expπΈ β πΈπππ
π πΈ βΉ 60 ππ/ππππππ
Fermi-Dirac Distribution
Source Channel Drain
p-typeDielectric
n-type
Gate
n-typex
π πΈ1π πΈ2
β expπΈ2 β πΈ1ππ
Decreased off current
Distribution of Electrons
πΈ2
πΈ1
SS limited to 60 ππ/ππππππ
MOSFET and TFET Structures
September 16, 20139
n-TFET
x
Energy distribution of holes
CB
VBOff-state currentX
Ener
gy
n-MOSFET
x
Energy distribution of electrons
thermal tail
CB
VB
Off-state current
Source Channel Drain Source Channel Drain
DielectricSource DrainGate
n-type n-typep-typex
DielectricSource DrainGate
p-type n-typeintrinsicx
Limited SS of ππππ½/π ππππ π No ππππ½/π ππππ π limit
Ener
gy
x
CB
VB
DielectricSource DrainGate
p-Si n-Sii-Sin-TFET
x
π β1
exp(π΄πππ)
Homostructure
September 16, 201310
x
CB
VB
DielectricSource DrainGate
p-GaSb n-InAsi-InAsn-TFET
x
HeterostructureTunneling in
Bilayer TFET Structure
September 16, 201313
+VD
p+ n+
Metal (+VG)Dielectric
(b)
MetalDielectric
(a)
iChannel
p+Source
n+Drain
Cut shown in (c)
DielectricMetal
BTBT
DielectricMetal (-VG)
Bottom
Gate
Top
Gate
(c)
πΈ1β
πΈ1π
Challenges Limiting TFET
Performance
Fundamental
Phonon effects
Band edge abruptness
Technological
Interface states
Complex geometries, design
Junction abruptness
Thickness variation with thin body
structures
Work function engineering
September 16, 201314
Summary
Frequency and voltage scaling of MOSFETs have stalled due to power constraints
Substantial voltage scaling requires new switching physics
TFETs employ tunneling to overcome 60 ππ/ππππππ limit
Experimental results have shown πΊπΊ < 60 ππ/ππππππ, albeit at low currents
Much work is still needed in matching theory to experiment
Heterojunctions and density-of-states switching designs may lead to better TFET performance
Weβre currently exploring the bilayer TFET, which utilizes an interesting device geometry to create electron and hole quantum wells
September 16, 201315