Transcript MOSFET Overview

Long Channel MOS Transistors
The theory developed for MOS capacitor (HO #2) can be
directly extended to Metal-Oxide-Semiconductor Field-Effect
transistors (MOSFET) by considering the following structure:
G
The gate bias, VG provides the
control of surface carrier
densities.
S
D
n+
n+
P
– For VG < Vth (threshold voltage),
the structure consists of two back to back diodes and only
leakage currents flow ( Io of PN junctions), i.e., ID  0
– For VG > Vth, inversion layer exists, a conducting channel
exists from D  S and current ID will flow.
Where Vth is determined by the properties of the structure.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 1
Long Channel MOS Transistors
Vth is given by Eq we derived for MOS capacitors. That is,
V th   ms 
Qf
C ox
 2B 
2qNa K s  o (2 B  VB )
(1)
C ox
where
ms  work funct ionbet ween met aland semiconduct or
Q f  int erfacechargedensit y
Cox  gat e oxide capacit ance
 B  bulk pot ent ial
N a  channeldoping concent ration
VB  subst rat ebias
n - channelMOSFETs: Vth  0
p - channelMOSFETs: Vth  0
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 2
1. NMOSFETs: Band Diagram
EF
VG  0  VD
VG  0
VD  0
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 3
NMOSFETs: Band Diagram
VG  Vth
VD  0
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 4
2. NMOSFETs: I - V Characteristics
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 5
NMOSFETs: I - V Characteristics
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 6
I  V Characteristics: Basic Equations
+VG
y
x
n+
QI(y)
+VD
ID
n+
QB(y)
P
Inversion
layer
Depletion
region
Note:
• The depletion region is wider around the drain because of the
applied drain voltage VD.
• The potential along the channel varies from VD @ y = L to 0 @
y = 0 between the drain and source.
• The channel charge QI and the bulk charge QB will in general
be f(y) because of the influence of VD, i.e. potential varies
along the channel length.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 7
I  V Characteristics: Basic Equations
1. Drain Current :
ID 
 J dydz  W  Q  E dy
x
I
n
x
2. Charge densityin thechannel:
QI ( y )  Cox VG  Vth ( y )
3.VG required t o induce inversion under theinfluenceof VD is :
1
Vth ( y )  V fb 
Cox
2 K s 0 qNa 2 B  VB  V ( y )   2B  V ( y )
where
W = width of the device
V(y) = voltage drop along the channel due to VD
Solving the above three Eq we get ID - VD characteristics.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 8
I  V Characteristics: Basic Equations
LinearRegion (VG  Vth , VD  VDSAT ) :
ID 
W
V 

 nCox VG  Vth  D VD
L
2

Saturation Region (VG  Vth , VD  VDSAT ) :
ID
W
 nCox VG  Vth 2
2L
VD = VDSAT
Linear
Region
VG6
Saturation
Region
VG5
VG4
VG3
VG2
VG1
VD
S. Saha
ID ((amps)1/2) 
ID 
VD (Volts)
HO #3: ELEN 384 - Review MOS Transistors
Page 9
3. MOS Device Scaling
Benefits of scaling MOSFETs:
1. increase
device
packing
density
L
xj
tox
n+
2. improve frequency response
(transit time)  1/L
n+
lo
P
3. improve current drive (transconductance, gm)
gm 
S. Saha
I D
VG
VD  constant

K 
W
 n ox 0 VD ,
L
tox

K 
W
 n ox 0 VG  Vth , forVD  VDSAT (saturation region)
L
tox
forVD  VDSAT (linearregion)
HO #3: ELEN 384 - Review MOS Transistors
Page 10
MOS Device Scaling
gm 
I D
VG
VD  constant
K ox 0
W
 n
VD ,
L
tox

forVD  VDSAT (linearregion)
K 
W
 n ox 0 VG  Vth , forVD  VDSAT (saturation region)
L
tox
• Note that gm and therefore, the current drive of MOSFETs
can be increased by:
– decreasing the channel length, L
– decreasing the gate oxide thickness, tox
• Therefore, much of the scaling is driven by decrease in L
and tox.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 11
MOS Device Scaling
Though, MOSFET scaling is driven by scaling down L and
tox, many problems such as increased electric fields are
encountered if scaled only these two parameters.
In 1974, Dennard et al. proposed a scaling methodology
which maintains the electric field in the device constants.
(R.H. Dennard, et al., IEEE JSSC, vol. 9, p. 256-268, 1974).
Device/circuit parameters
Constant field scaling factor
Dimension:
tox, L, W, xj, lo
Substrate doping:
Na
Supply voltage:
V
Supply current:
I
Parasitic capacitance: WL / tox
Gate delay:
CV / I
Power dissipation:
CV2 / delay
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
1/K
K
1/K
1/K
1/K
1/K
1/K2
Page 12
MOS Device Scaling
In practice, constant field scaling has not been strictly
observed. Since ID  gate overdrive, (VG – Vth), thus, the
demands for high performance have dictated the use of
higher supply voltage. However, high supply voltage implies
increased power dissipation (CV2f).
In the recent past, low power applications have become
important and have required a scaling scenario with lower
supply voltage.
Parameters
1970
1980
1990
2000
2006
Channel length (m)
10
4
1
0.18
0.10
Gate oxide (nm)
120
50
15
4
1.5
Junction depth (m)
>1
0.8
0.3
0.08
0.02-0.03
Supply voltage
12
5
3.3-5
1.5-1.8 0.6-0.9
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 13
MOS Device Scaling
Ref: B. Davari, et al., Proc.
IEEE, April 1995
Device/circuit parameters
Dimension:
Substrate doping:
Supply voltage:
S. Saha
Quasi Constant voltage scaling
(K > B > 1)
tox, L, W, xj, lo
Na
V
HO #3: ELEN 384 - Review MOS Transistors
1/K
K
1/B
Page 14
4. Limitations of Scaled MOSFETs
A number of factors have been neglected in the simple MOS
theory which became increasingly important in scaled
devices.
 bi, F, and ms of S/D junctions were neglected
– Vth dependence on W, L, and VD is not predicted by simple
theory
– I  0 for VG < Vth. Rather I is exponentially dependent on VG.
– Current flow D  S can be initiated by VD rather than VG.
This can be modeled by a Vth which depends on VD and VG.
– Since  fields cannot be held constant because of bi etc.
(and because VD has not been scaled in the industry),
higher   higher carrier velocity. Material limits like vsat
become important.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 15
4(a). Effect of Scaling Down L: Vth degradation
In long channel MOSFETs, the gate is completely
responsible for depleting the semiconductor (QB). In very
short devices, part of the depletion is accomplished by the
drain and source biases.
Since less VG is required to deplete QB, Vth as L. Similarly,
as VD, more QB is depleted by VD and hence Vth. This
effect dominates in lightly doped substrates.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 16
Effect of Scaling Down L: Punchthrough
If the channel length, L becomes too short, the depletion
region from the drain can reach source side reducing einjection barrier. This phenomenon is known as
punchthrough.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 17
Effect of Scaling Down L: DIBL
In very short channel
devices:
– less VG is required to
deplete QB
\ the barrier to electron
injection from source to
drain decreases.
– ID at a given VG.
This effect is known as
the drain induced barrier
lowering (DIBL).
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 18
Effect of Scaling L: Effect of DIBL on ID
• DIBL results in an increase in ID at a given VG. \ Vth as L.
Similarly, as VD, more QB is
depleted by VD and hence
Vth.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 19
4(b). Carrier Mobility: Velocity Saturation
The mobility of the carriers reduces at higher e-fields in
small channel length devices due to velocity saturation (vsat).
As L, while VD 
constant:
- lateral e-field
- carrier velocity 
vsat @ Ec  104
V/cm for e-.
\ for nMOSFETs with
L < 1 m, vsat causes
current to saturate for
VD < (VG  Vth).
\ I DSAT  WC ox (VG  Vth )vsat
Thus, I DSAT  (VG  Vth ) for short L devicesinsteadof square law.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 20
Effect of Vsat on MOSFET I - V Characteristics
MOSFETs with:
L = 2.7 um
tox = 500 A
(a)
(b)
(c)
(a) Experimental data; (b) simulated data including velocity
saturation; (c) simulated data ignoring velocity saturation.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 21
4(c). Sub-threshold Conduction
• For VG < Vth, the surface is in weak inversion and a
conducting channel starts to form. As a result, a low level of
current flows between the source and drain.
ID
VGS
In MOS subthreshold slope, S is limited to kT/q (60 mv/dec I)
\ ID leakage ; Static power ; and circuit instability .
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 22
4(d). Hot Carrier Effects
VG
n+ Source
Gate
Ig
l l l l l l
hot e l
m hole
VD > VDSAT
The maximum e-field
at the drain-substrate
junction is:
n+ Drain
Emax 
Isub
2qN a(i  VD )
K s 0
As L, in the channel
near the drain Emax
more rapidly than
long L devices.
The free carriers
passing through the
high e-field
gain
sufficient energy to
cause
hot-carrier
effects.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 23
Hot Carrier Effects
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 24
Hot Carrier Effects
• Isub flowing into the
substrate causes an
IR
drop
in
the
substrate resulting in
Body bias – Substrate
Current induced Body
Effect (SCBE).
– SCBE results in Vth
drop and manifold
increase in
S. Saha
HO #3: ELEN 384 - Review MOS Transistors

Isub

IDS.
Page 25
4(e). Band-to-Band Tunneling
• For small VG ~ 0 and high VD a significant drain leakage can be
observed, especially for short channel devices.
•
For VG = 0, and VD high, the e-field can be very high in the drain
region causing band-to-band tunneling (BTBT):
– BTBT happens only when e-field is sufficiently high to cause a
large band bending.

S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 26
4(f). Effect of Scaled Channel Width
The depletion region extends sideways in the areas outside
the gate controlled region increasing the apparent channel
width. As a result Vth opposite to short channel devices.
S. Saha
HO #3: ELEN 384 - Review MOS Transistors
Page 27