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EECS3611 Analog Integrated Circuit Design
Chapter 1
Introduction
EECS3611 Analog Integrated Circuit Design
Instructor: Prof. Ebrahim Ghafar-Zadeh,
Prof. Peter Lian
email: egz@cse.yorku.ca
peterlian@cse.yorku.ca
Course Web
https://wiki.eecs.yorku.ca/course_archive/2016-17/W/3611/
Schedule:
Lectures: PSE321, Mon. & Wed. 4:00pm – 5:30pm
Labs@BEL 334, Thur. 6:30pm-9:30pm,
Office hours:
Wed. 2:00-3:30pm@LAS1012C (starting Feb. 1, 2017)
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EECS3611 Analog Integrated Circuit Design
Textbook
Design of Analog CMOS Integrated Circuits
2nd Edition, Copyright: 2017
By: Behzad Razavi
McGraw Hill Education
ISBN-10: 0072524936
ISBN-13: 9780072524932
Available at York Bookstore
Grade Components
Assignment: 10%
Quiz: 15% (3 quizzes in class)
Lab: 25%
8 lab sessions
Starts on Jan. 26 (week 4, tentative)
Assessment based on lab report and design project.
Midterm 20%
Final 30%
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LAB
Lab will be at BEL 334
Lab contains two parts
Part 1 is for learning of EDA tool (i.e. Cadence), circuit
simulation, and layout.
Part 2 is for a design project.
Maintain a laboratory book or journal for all lab
sessions. It must be signed by the TA before you
leave the lab.
Topics covered
Introduction to analog design
Basic MOS device physics
Single state amplifiers
Layout and design rules
Differential amplifiers
Passive and active current mirrors
Frequency response of amplifiers
Noise
Feedback
Operational amplifiers
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Learning Outcomes
After successful completion of the course,
students are expected to be able to:
To analyze the characteristics of basic analog
integrated circuits
To formulate the behavior of basic analog circuits by
inspection
To perform circuit simulation using computer-aided
tool
To draw layout based on given design rules
EECS3611 Analog Integrated Circuit Design
Introduction
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Discrete Component and Integrated Circuits
Discrete component circuit (in EECS2210) consists of
different active components (transistors) and passive
components (capacitors, resistors and inductors).
Integrated circuit (this course) is a monolithic circuit
fabricated on a semiconductor substrate. It mainly
consists of transistors with limited number of resistors
and small value capacitors.
Discrete Component and Integrated Circuits
Discrete component circuit:
Both active and passive components are available.
Most are AC coupled circuit to isolate the DC biasing
points of different devices.
Low device density, high power consumption.
Integrated circuit:
Mainly transistors, as resistors and capacitors occupy
larger chip area.
Most are DC coupled circuit.
High device density, low power consumption.
High speed.
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Analog and Digital
Analog signal: Continuous in time and amplitude
Digital signal: discrete in time and amplitude
Analog signal Digital signal
Design of Analog and Digital Circuits
noise linearity
speed
power gain
I/O supply
impedance voltage
speed voltage
power
swing
Analog circuit Digital circuit
Multi trade-offs in analog design make it very complex.
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Why Analog?
Most of the physical signals are analog in nature
Need analog circuits to interface with physical
world
Why CMOS?
CMOS is now dominate the digital IC market:
Simple device structure, low fabrication cost.
Simple circuit for digital gates.
Advancement in CMOS technology.
Scalable and high integration density.
The demands for smaller and cheaper device, i.e.
monolithic circuit and System-on-Chip (SOC), drive
analog IC to CMOS technology.
To integrate analog and digital circuits into one chip.
To reduce the cost.
Analog IC is moving to CMOS technologies,
especially for low voltage and low power
applications.
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Passive Devices in CMOS
Resistor in CMOS:
Diffusion resistor: sheet resistance 100 Ω/ to
200Ω/
Poly silicon resistor: sheet resistance 20 Ω/ to
80Ω/
Well resistor: ~10kΩ/
Capacitor in CMOS:
PIP (poly-insulator-poly) capacitance: high linearity,
unit capacitance <1fF/µm2
MIM (metal-insulator-metal) capacitance: high linearity,
unit capacitance ~1fF/µm2
MOS capacitance: Use CG as capacitance– voltage
dependence
Large process variation: 20%.
Passive devices occupy larger silicon area
Analog IC Design Flow
System specifications
Tools Topology selection
Matlab Behavioral simulation
Hspice Circuit design & simulation
Virtuso Physical implementation (Layout)
Calibre Physical verification (DRC&LVS)
GDSII data out
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EECS3611 Analog Integrated Circuit Design
Review of MOSFET
MOSFET
MOSFET stands for Metal-Oxide-Semiconductor Field-
Effect Transistor.
A MOSFET comprises a Metal-Oxide-Semiconductor
stack
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MOSFET: 3D Structure
MOSFET Symbols
Two types of MOSFETs
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NMOS: Cutoff or Turned-Off
NMOS: Linear Region
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NMOS: Pinch-Off [VDS=VGS-Vth]
NMOS: Saturation [VDSVGS-Vth]
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NMOS Operation
NMOS: ID-VDS Characteristics
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NMOS: ID-VGS Characteristics
Body Effect
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Summary: Region of Operation
• Cut off region: VGS VTH
• Linear region: VGS VTH , VDS VGS -VTH
• Saturation region: VGS VTH , VDS VGS -VTH
Saturation region H
H
VTHN
L H
L H
L H
L H L
|VTHP|
Saturation region L
Linear region
Linear region
MOSFET: CMOS
CMOS stands for Complementary Metal-Oxide-
Semiconductor
Containing PMOS and NMOS transistors
P-channel device has opposite relative voltages,
has P+ source drains, and n-type substrate. Both
NMOS and PMOS devices are used in CMOS
technology.
P-channel device produces less
transconductance for similar dimension and
current compared to n-channel due to lower
mobility of holes.
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MOSFET: CMOS
Cross section of a NMOS and a PMOS FET in a CMOS
technology.
NMOS PMOS
EECS3611 Analog Integrated Circuit Design
Circuit Models
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Models for Design
Transistor is modeled using basic circuit
components.
Two types of models: large signal model and
small signal model
Large signal model – large signal low frequency,
such as DC bias points.
Small signal model – small signal and parameters
such as gain and frequency response of an analog
circuit.
MOSFET Model for Design
CGD
G D
CGS gmvgs gmbvbs ro
CGB
S CDB
CSB
B
A transistor is modeled by using four major components:
• A voltage controlled current source to model the
transconductance gm.
• Output resistance ro.
• A voltage controlled current source to model the back
gate transconductance gmb.
• Parasitic capacitance Cxx.
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Transistor DC Modeling
ID 0 for VGS VTH
W
I D μ Cox VGS - VTH VDS 1 VDS2 for VGS VTH , VDS VGS -VTH
L 2
1 W
ID μ Cox VGS - VTH 2 1 VDS for VGS VTH , VDS VGS -VTH
2 L
G D
where VGS - VTH VOD VDSAT .
ID ro
V TH = V TH 0 [ 2 F + V SB 2 F ]
Small Signal (AC) Model for Circuit Analysis
The model shown earlier is good for transistor
DC bias point calculation.
For AC analysis, a simple small signal model is
developed. In this analysis, a small AC signal v
is superimposed on normal DC biases.
In notation, AC signals will use all small letters,
DC all capitals and total voltage with AC and DC
components added will use mixed case
throughout this course. For example, VOUT is a
DC voltage, vout is an AC voltage and Vout is the
total voltage .
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Transconductance
The effect of gate voltage controlling the drain
current is modeled by transconductance
I D
gm
VGS
Hence this gm models how drain current will
change with change in gate voltage.
The transconductance is the most important
parameter of a transistor in analog circuit design.
This effect is modeled as a voltage controlled
current source between drain and source.
Transconductance
In the linear region, the transconductance of a MOSFET
is
W
g m Cox VDS
L
clearly indicating a drop with decreasing VDS.
In the saturation region
W W 2I D
g m Cox (VGS VTH ) 2 Cox I D
L L VGS VTH
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Output Conductance
The effect of the drain voltage is modeled using the output conductance
I D
gd
VDS
This models how ID changes when the VDS changes. Since we want only
input voltage to control ID and not the output voltage, ideally, this should
be zero.
Hence in saturation region using ID expression:
1 W I
I D Cox VGS - VTH (1 λVDS ) g d D I D
2
2 L VDS
This effect is captured as a resistance called output resistance:
1 1
ro
g d I D
Back Gate Transconductance
The effect of body bias or bulk voltage is modeled using
body or back gate transconductance.
I
g mb D
VBS
Hence this value is mainly determined by γ. This effect is
captured as a dependent current source circuit element
between drain and source.
I D
g mb gm g m
VBS 2 2 F VSB
Normally the back gate transconductance is 20% of the
front gate transconductance, i.e. η=0.2.
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MOSFET Capacitance
The fundamental mode of MOSFET operation is through
charge which is modeled through 3 non-linear bias
dependent capacitances CGS, CGD and CGB .
In addition, there are three linear overlap capacitances.
CGSO : Gate to source overlap capacitance per meter
of channel width. This and drain overlap capacitance
are independent of length L as they are associated
with edge effects.
CGDO : Similar to drain counterpart.
CGBO : Gate to bulk overlap capacitance per meter of
channel length and is associated with edge effects at
the width ends of the gate area.
MOS Structure Overlap Capacitance
lateral diffusion
Poly Gate
Source Drain
Top view n+ xd xd
W n+
Ldrawn
Gate
capacitance
S D
Depletion CGDO
CGSO
capacitance
Overlap capacitance (linear): CGSO CGDO COV W
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Total Gate Capacitance
Total gate capacitance in cut-off region: CGS CGSO
CGB is WLCox in series with Cd CGD CGDO
Cd is the depletion region capacitance (WLCox )Cd
CGB
(WLCox ) Cd
q si N A
Cd WL
4 F CGD
1
In linear region: CGS CGSO WLCox CDB
2
1
CGD CGDO WLCox
2
CGB 0
CGS
CSB
2
In saturation region: CGS CGSO WLCox
3
CGD CGDO CGB
CGB 0
Total Gate Capacitance
Cut off Saturation Linear
Total gate capacitance change in different
operation region.
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Junction Capacitance
CSB and CDB are capacitances between the
sidewalls and the bottom regions of the S and D
junctions.
S, D junction
S D E
W
CSB CDB
side wall bottom
Parasitic Capacitances
Since source – drain doping profiles are normally the same. We take drain
capacitance as an example.
For certain bias voltage VBD the drain-bulk capacitance is:
C DB 0
C DB MJ
VBD
1 -
PB
MJ Bulk junction sidewall capacitance grading coefficient
PB Bulk junction built-in potential
Zero bias drain capacitance CDB0 is:
C DB 0 Cbottom 0 Csidewall 0 AD C J W 2 E C JSW
CJ Zero bias bulk junction bottom capacitance per unit area
CJSW Zero bias bulk junction sidewall capacitance per meter of junction perimeter
E Drain width
AD Drain area from the layout
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Parasitic Resistances
RS and RD are the source and drain resistances
due to which inside source and drain voltages
applied to actual inversion layer will change for
high drain current.
In addition, there are noise coefficients which
may add some noise to ID.
This model ignores many parasitic resistances,
bipolar devices and PNPN devices.
Lumped Small Signal (AC) Model
The complete representation for NMOS and PMOS
devices is captured in the following figures.
All capacitors are lumped together.
For analytic calculations, this simple model is adequate.
Computer simulation tools like SPICE use more
sophisticated models that including hundreds of
parameters.
For low frequency analysis of the circuits, all capacitors
can be removed from the small signal model of the
transistor.
For full AC analysis, all elements are included in the
small signal model.
CGB and CGD can be removed as they are very small
compared to others in saturation region.
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Lumped Small Signal (AC) Model
CGD
G D
D
CGS
G gmvgs gmbvbs ro
CGB
S CDB
S
NMOS FET CSB
B
CGD
G D
D
CGS
G gmvgs gmbvbs ro
CGB
S CDB
S
PMOS FET CSB
B
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