Title: OUTLINE
1Lecture 34
- OUTLINE
- The MOS Capacitor
- MOS non-idealities (cont.)
- VT adjustment
- Reading Chapter 18.3
2Poly-Si Gate Depletion
- A heavily doped film of polycrystalline silicon
(poly-Si) is typically employed as the
gate-electrode material in modern MOS devices. - There are practical limits to the electrically
active dopant concentration (usually less than
1x1020 cm-3) - The gate must be considered as a semiconductor,
rather than a metal
NMOS
PMOS
3MOS Band Diagram with Gate Depletion
Si biased to inversion
WT
VG is effectively reduced
Ec
EFS
qfS
Ev
qVG
qVpoly
Ec
Ev
Wpoly
How can gate depletion be minimized?
P-type Si
N poly-Si gate
4Gate Depletion Effect
Gausss Law dictates
e
qN
W
/
E
xo is effectively increased
poly
ox
ox
poly
N poly-Si
Cpoly
Cox
N
p-type Si
5Example GDE
Vox , the voltage across a 2 nm thin oxide, is 1
V. The n poly-Si gate active dopant
concentration Npoly is 8 ?1019 cm-3 and the Si
substrate doping concentration NA is 1017cm-3.
Find (a) Wpoly , (b) Vpoly , and (c) VT .
Solution (a)
e
e
/
/
qN
x
V
qN
W
E
poly
o
ox
ox
poly
ox
ox
poly
-
14
V
1
)
F/cm
(
10
85
.
8
9
.
3
-
-
-
3
19
19
7
cm
10
8
C
10
6
.
1
cm
10
2
nm
3
.
1
6(b)
(c)
Is the loss of 0.11V significant?
7Inversion-Layer Thickness Tinv
The average inversion-layer location below the
Si/SiO2 interface is called the inversion-layer
thickness, Tinv .
Si
SiO2
poly-Si gate
-50
-40
-30
-20
-10
0
10
20
30
40
50
8Effective Oxide Thickness, Toxe
at VGVdd
(VG VT)/Toxe can be shown to be the average
electric field in the inversion layer. Tinv of
holes is larger than that of electrons because of
the difference in effective masses.
9Effective Oxide Capacitance, Coxe
C
Basic LF C-V
C
ox
with gate-depletion
with gate-depletion and
charge-layer thickness
data
V
G
10VT Adjustment by Ion Implantation
- In modern IC fabrication processes, the threshold
voltages of MOS transistors are adjusted by ion
implantation - A relatively small dose NI (units ions/cm2) of
dopant atoms is implanted into the near-surface
region of the semiconductor - When the MOS device is biased in depletion or
inversion, the implanted dopants add to the
dopant-ion charge near the oxide-semiconductor
interface.