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8/12/2019 VLSI Design Lab1 by Parag
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VLSI Design Lab
Presented By:
Parag Parandkar
Associate Professor, ECE Department,
Oriental University, Indore
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Types of IC Designs
IC Designs can be Analogor Digital
Digital designs can be one of three groups
Full Custom Every transistor designed and laid out by hand
ASIC (Application-Specific Integrated Circuits) Designs synthesized automatically from a high-level
language description
Semi-Custom Mixture of custom and synthesized modules
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Need for transistors
Cannot make logic gates with voltage/currentsource, RLC components Consider steady state behavior of L and C
Need a switch: something where a (small)
signal can control the flow of another signal
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Introduction to
CMOS VLSIDesign
CMOS Transistor Theory
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Introduction So far, we have treated transistors as ideal switches
An ON transistor passes a finite amount of current Depends on terminal voltages
Derive current-voltage (I-V) relationships
Transistor gate, source, drain all have capacitance I = C (dV/dt) -> dt = (C/I) dV
Capacitance and current determine speed
Also explore what a degraded level really means
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MOS Capacitor
Gate and body form MOS capacitor
Operating modes Accumulation
Depletion
Inversion
polysilicon gate
(a)
silicon dioxide insulator
p-type body+-
Vg< 0
(b)
+-
0 < Vg< V
t
depletion region
(c)
+-
Vg> V
t
depletion region
inversion region
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Terminal Voltages Mode of operation depends on Vg, Vd, Vs
Vgs= VgVs Vgd= VgVd Vds= VdVs= Vgs- Vgd
Source and drain are symmetric diffusion terminals
By convention, source is terminal at lower voltage
Hence Vds0
nMOS body is grounded. First assume source is 0 too.
Three regions of operation
Cutoff
Linear
Saturation
Vg
Vs
Vd
Vgd
Vgs
Vds
+-
+
-
+
-
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nMOS Cutoff
No channel
Ids= 0
+-
Vgs
= 0
n+ n+
+-
Vgd
p-type body
b
g
s d
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nMOS Linear Channel forms
Current flows from d to s e-from s to d
Idsincreases with Vds Similar to linear resistor
+-
Vgs
> Vt
n+ n+
+-
Vgd
= Vgs
+
-
Vgs
> Vt
n+ n+
+
-
Vgs
> Vgd
> Vt
Vds= 0
0 < Vds
< Vgs
-Vt
p-type body
p-type body
b
g
s d
b
g
s dIds
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nMOS Saturation
Channel pinches off Idsindependent of Vds We say current saturates
Similar to current source
+-
Vgs
> Vt
n+ n+
+-
Vgd
< Vt
Vds> Vgs-Vt
p-type body
b
g
s d Ids
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I-V Characteristics
In Linear region, Idsdepends on How much charge is in the channel?
How fast is the charge moving?
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Channel Charge
MOS structure looks like parallel platecapacitor while operating in inversion Gateoxidechannel
Qchannel=
n+ n+
p-type body
+
Vgd
gate
+ +
source
-
Vgs-
drain
Vds
channel-
Vg
Vs
Vd
Cg
n+ n+
p-type body
W
L
tox
SiO2gate oxide
(good insulator, ox
= 3.9)
polysilicon
gate
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Channel Charge
MOS structure looks like parallel platecapacitor while operating in inversion Gateoxidechannel
Qchannel
= CV
C = Cg= eoxWL/tox= CoxWL
V = VgcVt= (VgsVds/2)Vt
n+ n+
p-type body
+
Vgd
gate
+ +source
-
Vgs
-drain
Vds
channel-
Vg
Vs
Vd
Cg
n+ n+
p-type body
W
L
tox
SiO2gate oxide
(good insulator, ox
= 3.9)
polysilicon
gate
Cox= eox/ tox
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Channel Charge MOS structure looks like parallel plate
capacitor while operating in inversion Gateoxidechannel
Qchannel= CV
C = Cg= eoxWL/tox= CoxWL
V =
n+ n+
p-type body
+
Vgd
gate
+ +
source
-
Vgs-
drain
Vds
channel-
Vg
Vs
Vd
Cg
n+ n+
p-type body
W
L
tox
SiO2gate oxide
(good insulator, ox
= 3.9)
polysilicon
gate
Cox= eox/ tox
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Channel Charge MOS structure looks like parallel plate
capacitor while operating in inversion Gateoxidechannel
Qchannel= CV
C = Cg= eoxWL/tox= CoxWL
V = VgcVt= (VgsVds/2)Vt
n+ n+
p-type body
+
Vgd
gate
+ +
source
-
Vgs
-drain
Vds
channel-
Vg
Vs
Vd
Cg
n+ n+
p-type body
W
L
tox
SiO2gate oxide
(good insulator, ox
= 3.9)
polysilicon
gate
Cox= eox/ tox
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Carrier velocity
Charge is carried by e-
Carrier velocity vproportional to lateral E-field between source and drain
v== mE m called mobility
E = Vds/L
Time for carrier to cross channel: t= L / v
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nMOS Linear I-V
Now we know How much charge Qchannelis in the channel
How much time teach carrier takes to cross
dsI
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nMOS Linear I-V
Now we know How much charge Qchannelis in the channel
How much time teach carrier takes to crosschannel
dsQI
t
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nMOS Linear I-V
Now we know How much charge Qchannelis in the channel
How much time teach carrier takes to cross
channel
ox 2
2
ds
dsgs t ds
dsgs t ds
QIt
W VC V V V
L
VV V V
ox=
WC
L
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nMOS Saturation I-V
If Vgd< Vt, channel pinches off near drain When Vds> Vdsat= VgsVt
Now drain voltage no longer increases current
dsI
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nMOS Saturation I-V
If Vgd< Vt, channel pinches off near drain When Vds> Vdsat= VgsVt
Now drain voltage no longer increases current
2dsat
ds gs t dsat
VI V V V
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nMOS Saturation I-V
If Vgd< Vt, channel pinches off near drain When Vds> Vdsat= VgsVt
Now drain voltage no longer increases current
2
2
2
dsatds gs t dsat
gs t
VI V V V
V V
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nMOS I-V Summary
2
cutoff
linear
saturatio
0
2
2n
gs t
dsds gs t ds ds dsat
gs t ds dsat
V V
VI V V V V V
V V V V
Shockley1storder transistor models
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Example Example: a 0.6 mm process from AMI
semiconductor tox= 100
m = 350 cm2/V*s
Vt= 0.7 V Plot Idsvs. Vds
Vgs= 0, 1, 2, 3, 4, 5
Use W/L = 4/2 l
14
2
8
3.9 8.85 10350 120 /
100 10ox
W W WC A V
L L L
0 1 2 3 4 50
0.5
1
1.5
2
2.5
Vds
Ids
(mA)
Vgs
= 5
Vgs
= 4
Vgs
= 3
Vgs
= 2
Vgs= 1
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pMOS I-V
All dopings and voltages are inverted forpMOS
Mobility mp
is determined by holes Typically 2-3x lower than that of electrons mn 120 cm2/V*s in AMI 0.6 mm process
Thus pMOS must be wider to provide samecurrent In this class, assume mn/ mp= 2
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Capacitance
Any two conductors separated by an insulatorhave capacitance
Gate to channel capacitor is very important Creates channel charge necessary for operation
Source and drain have capacitance to body Across reverse-biased diodes
Called diffusion capacitance because it isassociated with source/drain diffusion
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Gate Capacitance Approximate channel as connected to source
Cgs= eoxWL/tox= CoxWL = CpermicronW
Cpermicronis typically about 2 fF/mm
n+ n+
p-type body
W
Ltox
SiO2gate oxide
(good insulator, ox
= 3.90)
polysilicon
gate
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Diffusion Capacitance
Csb, Cdb Undesirable, calledparasiticcapacitance
Capacitance depends on area and perimeter Use small diffusion nodes
Comparable to Cg
for contacted diff
Cgfor uncontacted
Varies with process
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Pass Transistors
We have assumed source is grounded
What if source > 0? e.g. pass transistor passing V
DD
VDD
VDD
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Pass Transistors
We have assumed source is grounded What if source > 0?
e.g. pass transistor passing VDD
Vg= VDD If Vs> VDD-Vt, Vgs< Vt Hence transistor would turn itself off
nMOS pass transistors pull no higher than VDD-Vtn
Called a degraded 1 Approach degraded value slowly (low Ids)
pMOS pass transistors pull no lower than Vtp
VDD
VDD
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Pass Transistor Ckts
VDD
VDD
VSS
VDD
VDD
VDD
VDD
VDD
VDD
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Pass Transistor Ckts
VDD
VDD V
s
= VDD
-Vtn
VSS
Vs= |V
tp|
VDD
VDD-Vtn VDD-VtnV
DD-V
tn
VDD
VDD
VDD
VDD
VDD
VDD
-Vtn
VDD-2Vtn
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Back to Introduction Integrated circuits: many transistors on one chip. Very Large Scale Integration(VLSI): very many Complementary Metal Oxide Semiconductor
Fast, cheap, low power transistors
Today: How to build your own simple CMOSchip CMOS transistors Building logic gates from transistors Transistor layout and fabrication
Rest of the course: How to build a good CMOSchip
nMOS Transistor
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nMOS Transistor Four terminals: gate, source, drain, body
Gateoxidebody stack looks like a capacitor Gate and body are conductors
SiO2(oxide) is a very good insulator
Called metaloxidesemiconductor (MOS)capacitor
Even though gate is
no longer made of metal
n+
p
GateSource Drain
bulk Si
SiO2
Polysilicon
n+
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nMOS Operation
Body is commonly tied to ground (0 V) When the gate is at a low voltage:
P-type body is at low voltage
Source-body and drain-body diodes are OFFNo current flows, transistor is OFF
n+
p
GateSource Drain
bulk Si
SiO2
Polysilicon
n+D
0
S
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nMOS Operation Cont.
When the gate is at a high voltage: Positive charge on gate of MOS capacitor
Negative charge attracted to body
Inverts a channel under gate to n-type
Now current can flow through n-type silicon fromsource through channel to drain, transistor is ON
n+
p
GateSource Drain
bulk Si
SiO2
Polysilicon
n+
D
1
S
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pMOS Transistor
Similar, but doping and voltages reversed Body tied to high voltage (VDD)
Gate low: transistor ON
Gate high: transistor OFF
Bubble indicates inverted behavior
SiO
2
n
GateSource Drain
bulk Si
Polysilicon
p+ p+
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Power Supply Voltage
GND = 0 V
In 1980s, VDD= 5V
VDDhas decreased in modern processes High VDDwould damage modern tiny transistors
Lower VDDsaves power
VDD= 3.3, 2.5, 1.8, 1.5, 1.2, 1.0,
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Transistors as Switches We can view MOS transistors as electrically
controlled switches
Voltage at gate controls path from source todrain
g
s
d
g = 0
s
d
g = 1
s
d
g
s
d
s
d
s
d
nMOS
pMOS
OFFON
ONOFF
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CMOS Inverter
A Y
0
1
VDD
A Y
GNDA Y
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CMOS Inverter
A Y
0
1 0
VDD
A=1 Y=0
GND
ON
OFF
A Y
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CMOS Inverter
A Y
0 1
1 0
VDD
A=0 Y=1
GND
OFF
ON
A Y
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CMOS NAND Gate
A B Y
0 0
0 1
1 0
1 1
A
B
Y
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CMOS NAND Gate
A B Y
0 0 1
0 1
1 0
1 1
A=0
B=0
Y=1
OFF
ON ON
OFF
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CMOS NAND Gate
A B Y
0 0 1
0 1 1
1 0
1 1
A=0
B=1
Y=1
OFF
OFF ON
ON
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CMOS NAND Gate
A B Y
0 0 1
0 1 1
1 0 1
1 1
A=1
B=0
Y=1
ON
ON OFF
OFF
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CMOS NAND Gate
A B Y
0 0 1
0 1 1
1 0 1
1 1 0
A=1
B=1
Y=0
ON
OFF OFF
ON
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CMOS NOR Gate
A B Y
0 0 1
0 1 0
1 0 0
1 1 0
A
BY
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3-input NAND Gate
Y pulls low if ALL inputs are 1
Y pulls high if ANY input is 0
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3-input NAND Gate
Y pulls low if ALL inputs are 1
Y pulls high if ANY input is 0
A
B
Y
C
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CMOS Fabrication
CMOS transistors are fabricated on siliconwafer
Lithography process similar to printing press
On each step, different materials are depositedor etched
Easiest to understand by viewing both top andcross-section of wafer in a simplifiedmanufacturing process
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Inverter Cross-section Typically use p-type substrate for nMOS
transistors
Requires n-well for body of pMOS transistors
n+
p substrate
p+
n well
A
YGND V
DD
n+ p+
SiO2
n+ diffusion
p+ diffusion
polysilicon
metal1
nMOS transistor pMOS transistor
Well and Substrate Taps
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Well and Substrate Taps Substrate must be tied to GND and n-well to
VDD Metal to lightly-doped semiconductor forms
poor connection called Shottky Diode
Use heavily doped well and substrate contacts/ taps
n+
p substrate
p+
n well
A
YGND V
DD
n+p+
substrate tap well tap
n+ p+
I M k S
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Inverter Mask Set
Transistors and wires are defined by masks Cross-section taken along dashed line
GND VDD
Y
A
substrate tap well tap
nMOS transistor pMOS transistor
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Detailed Mask Views
Six masks n-well
Polysilicon
n+ diffusion
p+ diffusion
Contact
MetalMetal
Polysilicon
Contact
n+ Diffusion
p+ Diffusion
n well
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Fabrication Steps
Start with blank wafer
Build inverter from the bottom up
First step will be to form the n-well Cover wafer with protective layer of SiO2(oxide)
Remove layer where n-well should be built
Implant or diffuse n dopants into exposed wafer
Strip off SiO2
p substrate
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Oxidation
Grow SiO2on top of Si wafer 9001200 C with H2O or O2in oxidation furnace
p substrate
SiO2
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Photoresist
Spin on photoresist Photoresist is a light-sensitive organic polymer
Softens where exposed to light
p substrate
SiO2
Photoresist
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Lithography
Expose photoresist through n-well mask
Strip off exposed photoresist
p substrate
SiO2
Photoresist
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Etch
Etch oxide with hydrofluoric acid (HF) Seeps through skin and eats bone; nasty stuff!!!
Only attacks oxide where resist has been
exposed
p substrate
SiO2
Photoresist
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Strip Photoresist
Strip off remaining photoresist Use mixture of acids called piranah etch
Necessary so resist doesnt melt in next step
p substrate
SiO2
n-well
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n-well is formed with diffusion or ionimplantation
Diffusion Place wafer in furnace with arsenic gas
Heat until As atoms diffuse into exposed Si
Ion Implanatation Blast wafer with beam of As ions
Ions blocked by SiO2, only enter exposed Si
n well
SiO2
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Strip Oxide
Strip off the remaining oxide using HF
Back to bare wafer with n-well
Subsequent steps involve similar series ofsteps
p substrate
n well
Pol silicon
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Polysilicon Deposit very thin layer of gate oxide
< 20 (6-7 atomic layers) Chemical Vapor Deposition (CVD) of silicon
layer
Place wafer in furnace with Silane gas (SiH4) Forms many small crystals called polysilicon
Heavily doped to be good conductor
Thin gate oxide
Polysilicon
p substraten well
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Polysilicon Patterning
Use same lithography process to patternpolysilicon
Polysilicon
p substrate
Thin gate oxidePolysilicon
n well
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Self-Aligned Process
Use oxide and masking to expose where n+dopants should be diffused or implanted
N-diffusion forms nMOS source, drain, and n-
well contact
p substraten well
N diff sion
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N-diffusion Pattern oxide and form n+ regions
Self-aligned processwhere gate blocksdiffusion
Polysilicon is better than metal for self-alignedgates because it doesnt melt during later
processing
p substraten well
n+ Diffusion
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N-diffusion cont.
Historically dopants were diffused
Usually ion implantation today
But regions are still called diffusion
n wellp substrate
n+n+ n+
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N-diffusion cont.
Strip off oxide to complete patterning step
n wellp substrate
n+n+ n+
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P-Diffusion
Similar set of steps form p+ diffusion regionsfor pMOS source and drain and substratecontact
p+ Diffusion
p substraten well
n+n+ n+p+p+p+
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Contacts
Now we need to wire together the devices Cover chip with thick field oxide
Etch oxide where contact cuts are needed
p substrate
Thick field oxide
n well
n+n+ n+p+p+p+
Contact
Metalization
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Metalization Sputter on aluminum over whole wafer
Pattern to remove excess metal, leaving wires
p substrate
Metal
Thick field oxide
n well
n+n+ n+p+p+p+
Metal
Layout
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Layout Chips are specified with set of masks
Minimum dimensions of masks determinetransistor size (and hence speed, cost, and power)
Feature sizef= distance between source and drain Set by minimum width of polysilicon
Feature size improves 30% every 3 years or so
Normalize for feature size when describing design
rules Express rules in terms of l =f/2
E.g. l = 0.3 mm in 0.6 mm process
Simplified Design Rules
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Simplified Design Rules
Conservative rules to get you started
Inverter Layout
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y Transistor dimensions specified as Width /
Length Minimum size is 4l / 2l, sometimes called 1 unit
Inf= 0.6 mm process, this is 1.2 mm wide, 0.6 mmlong
S
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Summary
MOS Transistors are stack of gate, oxide, silicon Can be viewed as electrically controlled switches
Build logic gates out of switches
Draw masks to specify layout of transistors
Now you know everything necessary to start
designing schematics and layout for a simplechip!
SYSTEMFPGA Cell Based
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MODULE
LOGIC GATE
CIRCUIT
D Q
CMOS Inverter
ASIC
Full-Custom
FPGA
PLD
Cell-Based
Gate
Arrays
X
Combinational SequentialR
E
G
DECODER
M
U
X
Simple
Basic
Complex
StaticDynamic
Parallel
Connection
Series
Connection
pn n+ +
MOSFETBipolar Diode
n pn+ n+p
DEVICE
Copy Right
August 2002
Maitham Shams
The MOSFET
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Maitham Shams2002
n+ n+
Gate OxideSource Drain
Body
p-substrate
Gate
2Thin Oxide (SiO2))Polycrystalline Silicon
or Polysilicon (conductor)
Lightly doped
Bulk Contact
FieldOxide
p+ p+
Channel stop implantor field implant
2Thick Oxide (SiO2)
Heavily doped byimplantation or diffusion
For insulatingdevices from
each other
Metal-Oxide-Semiconductor Field-Effect Transistor
Unipolar and symmetric device with four terminals of Gate, Source, Drain, and Body
NMOS: n-type Source and Drain, p-type Body connected to ground (GND)
PMOS: p-type Source and Drain, n-type Body connected to power supply (VDD)
CMOS Technology
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Maitham Shams2002
PMOS NMOS
p+ n+ n+
p-substrate
p+
contact cut
Polysilicon
n-well
MetalGate oxide
Complementary Metal Oxide Silicon Technology combines NMOS and PMOS
Mainstream IC Technology
in
Foreseeable Future
High Integration
Density
Simple Processing
Steps
Low PowerConsumption
Adequate SpeedHigh Reliability
MOSFET Types and Symbols
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D
G
S
D
G
S
D
G
S
D
G
S
B
Analog Digital With non standardsubstrate connection
Enhancement PMOS Depletion PMOS
IDS
VGS +VTp
0
IDS
VGS
-VTp0
D
G
S
D
G
S
D
G
S
B
D
G
S
Analog Digital With non standardsubstrate connection
Enhancement NMOS Depletion NMOS
IDS
VGS+VTn0
0
IDS
VGS-VTn
Enhancement mode transistors are normally OFF (non-conducting with zero bias)
Depletion mode transistors are normally ON (conduct with zero bias)
Most CMOS ICs use Enhancement type MOS