Introduction to CMOS VLSI Design MOS devices: static and dynamic behavior.

Slides:



Advertisements
Similar presentations
EE 447 VLSI Design Lecture 7: Combinational Circuits
Advertisements

Introduction to CMOS VLSI Design Combinational Circuits
Design and Implementation of VLSI Systems (EN1600)
Logic Gate Delay Modeling -1 Bishnu Prasad Das Research Scholar CEDT, IISc, Bangalore
Topics Electrical properties of static combinational gates:
Elettronica T A.A Digital Integrated Circuits © Prentice Hall 2003 Inverter CMOS INVERTER.
Transistor nMOS Q channel = CV C = C g =  ox WL/t ox = C ox WL V = V gc – V t = (V gs – V ds /2) – V t v =  E  (mobility) E = V ds /L Time for carrier.
DC Characteristics of a CMOS Inverter
DC Response DC Response: Vout vs. Vin for a gate Ex: Inverter
Lecture 5: DC & Transient Response
Lecture 9: Combinational Circuit Design. CMOS VLSI DesignCMOS VLSI Design 4th Ed. 10: Combinational Circuits2 Outline  Bubble Pushing  Compound Gates.
A Look at Chapter 4: Circuit Characterization and Performance Estimation Knowing the source of delays in CMOS gates and being able to estimate them efficiently.
S. RossEECS 40 Spring 2003 Lecture 21 CMOS INVERTER CMOS means Complementary MOS: NMOS and PMOS working together in a circuit D S V DD (Logic 1) D S V.
Introduction to CMOS VLSI Design Lecture 3: CMOS Transistor Theory David Harris Harvey Mudd College Spring 2004.
CMOS Transistor and Circuits
Introduction to CMOS VLSI Design Lecture 5 CMOS Transistor Theory
VLSI Design CMOS Transistor Theory. EE 447 VLSI Design 3: CMOS Transistor Theory2 Outline Introduction MOS Capacitor nMOS I-V Characteristics pMOS I-V.
S. RossEECS 40 Spring 2003 Lecture 22 Inside the CMOS inverter, no I D current flows through transistors when input is logic 1 or logic 0, because the.
Introduction to CMOS VLSI Design Combinational Circuits.
Z. Feng MTU EE4800 CMOS Digital IC Design & Analysis Fall EE4800 CMOS Digital IC Design & Analysis Lecture 7 Midterm Review Zhuo Feng.
Introduction to CMOS VLSI Design Lecture 4: DC & Transient Response
Introduction to CMOS VLSI Design Lecture 4: DC & Transient Response Credits: David Harris Harvey Mudd College (Material taken/adapted from Harris’ lecture.
CMOS Digital Integrated Circuits 1 Lec 7 CMOS Inverters: Dynamic Analysis and Design.
Lecture #24 Gates to circuits
Introduction to CMOS VLSI Design Lecture 3: CMOS Transistor Theory
Design and Implementation of VLSI Systems (EN0160) Prof. Sherief Reda Division of Engineering, Brown University Spring 2007 [sources: Weste/Addison Wesley.
S. Reda EN160 SP’07 Design and Implementation of VLSI Systems (EN0160) Lecture 22: Material Review Prof. Sherief Reda Division of Engineering, Brown University.
Outline Noise Margins Transient Analysis Delay Estimation
DC and transient responses Lezione 3
S. Reda EN160 SP’07 Design and Implementation of VLSI Systems (EN0160) Lecture10: Delay Estimation Prof. Sherief Reda Division of Engineering, Brown University.
S. Reda VLSI Design Design and Implementation of VLSI Systems (EN1600) lecture09 Prof. Sherief Reda Division of Engineering, Brown University Spring 2008.
CMOS VLSI Design4: DC and Transient ResponseSlide 1 EE466: VLSI Design Lecture 05: DC and transient response – CMOS Inverters.
EE4800 CMOS Digital IC Design & Analysis
Introduction to CMOS VLSI Design Lecture 4: DC & Transient Response Greco/Cin-UFPE (Material taken/adapted from Harris’ lecture notes)
© 2000 Prentice Hall Inc. Figure 6.1 AND operation.
EE 447 VLSI Design 4: DC and Transient Response1 VLSI Design DC & Transient Response.
Transistor Characteristics EMT 251. Outline Introduction MOS Capacitor nMOS I-V Characteristics (ideal) pMOS I-V Characteristics (ideal)
The CMOS Inverter Slides adapted from:
Digital Integrated Circuits© Prentice Hall 1995 Inverter THE INVERTERS.
MOS Inverter: Static Characteristics
1 Delay Estimation Most digital designs have multiple data paths some of which are not critical. The critical path is defined as the path the offers the.
Mary Jane Irwin ( ) Modified by Dr. George Engel (SIUE)
Mary Jane Irwin ( ) CSE477 VLSI Digital Circuits Fall 2002 Lecture 04: CMOS Inverter (static view) Mary Jane.
Dec 2010Performance of CMOS Circuits 1 Instructed by Shmuel Wimer Eng. School, Bar-Ilan University Credits: David Harris Harvey Mudd College (Some material.
THE INVERTERS. DIGITAL GATES Fundamental Parameters l Functionality l Reliability, Robustness l Area l Performance »Speed (delay) »Power Consumption »Energy.
Chapter 07 Electronic Analysis of CMOS Logic Gates
Modern VLSI Design 2e: Chapter 3 Copyright  1998 Prentice Hall PTR Topics n Electrical properties of static combinational gates: –transfer characteristics;
Device Characterization ECE/ChE 4752: Microelectronics Processing Laboratory Gary S. May April 1, 2004.
Introduction to CMOS VLSI Design Lecture 6: Logical Effort
Linear Delay Model In general the propagation delay of a gate can be written as: d = f + p –p is the delay due to intrinsic capacitance. –f is the effort.
EE141 © Digital Integrated Circuits 2nd Devices 1 Goal of this lecture  Present understanding of device operation  nMOS/pMOS as switches  How to design.
Digital Integrated Circuits A Design Perspective
Lecture 20 Today we will Look at why our NMOS and PMOS inverters might not be the best inverter designs Introduce the CMOS inverter Analyze how the CMOS.
Solid-State Devices & Circuits
Chapter 6 Copyright © 2004 The McGraw-Hill Companies, Inc. All rights reserved. High-Speed CMOS Logic Design.
Circuit Delay Performance Estimation Most digital designs have multiple signal paths and the slowest one of these paths is called the critical path Timing.
Introduction to CMOS VLSI Design CMOS Transistor Theory
7-1 Integrated Microsystems Lab. EE372 VLSI SYSTEM DESIGNE. Yoon MOS Inverter — All essential features of MOS logic gates DC and transient characteristics.
Wujie Wen, Assistant Professor Department of ECE
COE 360 Principles of VLSI Design Delay. 2 Definitions.
CMOS VLSI Design Lecture 4: DC & Transient Response Younglok Kim Sogang University Fall 2006.
VLSI System Design DC & Transient Response
Introduction to CMOS VLSI Design Chapter 4 Delay
DC & Transient Response
Introduction to CMOS VLSI Design Lecture 5: DC & Transient Response
UNIT-II Stick Diagrams
Lecture 5: DC & Transient Response
Introduction to CMOS VLSI Design Lecture 4: DC & Transient Response
Presentation transcript:

Introduction to CMOS VLSI Design MOS devices: static and dynamic behavior

CMOS VLSI DesignMOS equationsSlide 2 Outline  DC Response  Logic Levels and Noise Margins  Transient Response  Delay Estimation

CMOS VLSI DesignMOS equationsSlide 3 Activity 1) If the width of a transistor increases, the current will increasedecreasenot change 2) If the length of a transistor increases, the current will increasedecreasenot change 3) If the supply voltage of a chip increases, the maximum transistor current will increasedecreasenot change 4) If the width of a transistor increases, its gate capacitance will increasedecreasenot change 5) If the length of a transistor increases, its gate capacitance will increasedecreasenot change 6) If the supply voltage of a chip increases, the gate capacitance of each transistor will increasedecreasenot change

CMOS VLSI DesignMOS equationsSlide 4 Activity 1) If the width of a transistor increases, the current will increasedecreasenot change 2) If the length of a transistor increases, the current will increasedecreasenot change 3) If the supply voltage of a chip increases, the maximum transistor current will increasedecreasenot change 4) If the width of a transistor increases, its gate capacitance will increasedecreasenot change 5) If the length of a transistor increases, its gate capacitance will increasedecreasenot change 6) If the supply voltage of a chip increases, the gate capacitance of each transistor will increasedecreasenot change

CMOS VLSI DesignMOS equationsSlide 5 DC Response  DC Response: V out vs. V in for a gate  Ex: Inverter –When V in = 0 -> V out = V DD –When V in = V DD -> V out = 0 –In between, V out depends on transistor size and current –By KCL, must settle such that I dsn = |I dsp | –We could solve equations –But graphical solution gives more insight

CMOS VLSI DesignMOS equationsSlide 6 Transistor Operation  Current depends on region of transistor behavior  For what V in and V out are nMOS and pMOS in –Cutoff? –Linear? –Saturation?

CMOS VLSI DesignMOS equationsSlide 7 nMOS Operation CutoffLinearSaturated V gsn <V gsn > V dsn < V gsn > V dsn >

CMOS VLSI DesignMOS equationsSlide 8 nMOS Operation CutoffLinearSaturated V gsn < V tn V gsn > V tn V dsn < V gsn – V tn V gsn > V tn V dsn > V gsn – V tn

CMOS VLSI DesignMOS equationsSlide 9 nMOS Operation CutoffLinearSaturated V gsn < V tn V gsn > V tn V dsn < V gsn – V tn V gsn > V tn V dsn > V gsn – V tn V gsn = V in V dsn = V out

CMOS VLSI DesignMOS equationsSlide 10 nMOS Operation CutoffLinearSaturated V gsn < V tn V in < V tn V gsn > V tn V in > V tn V dsn < V gsn – V tn V out < V in - V tn V gsn > V tn V in > V tn V dsn > V gsn – V tn V out > V in - V tn V gsn = V in V dsn = V out

CMOS VLSI DesignMOS equationsSlide 11 pMOS Operation CutoffLinearSaturated V gsp >V gsp < V dsp > V gsp < V dsp <

CMOS VLSI DesignMOS equationsSlide 12 pMOS Operation CutoffLinearSaturated V gsp > V tp V gsp < V tp V dsp > V gsp – V tp V gsp < V tp V dsp < V gsp – V tp

CMOS VLSI DesignMOS equationsSlide 13 pMOS Operation CutoffLinearSaturated V gsp > V tp V gsp < V tp V dsp > V gsp – V tp V gsp < V tp V dsp < V gsp – V tp V gsp = V in - V DD V dsp = V out - V DD V tp < 0

CMOS VLSI DesignMOS equationsSlide 14 pMOS Operation CutoffLinearSaturated V gsp > V tp V in > V DD + V tp V gsp < V tp V in < V DD + V tp V dsp > V gsp – V tp V out > V in - V tp V gsp < V tp V in < V DD + V tp V dsp < V gsp – V tp V out < V in - V tp V gsp = V in - V DD V dsp = V out - V DD V tp < 0

CMOS VLSI DesignMOS equationsSlide 15 I-V Characteristics  Make pMOS is wider than nMOS such that  n =  p

CMOS VLSI DesignMOS equationsSlide 16 Current vs. V out, V in

CMOS VLSI DesignMOS equationsSlide 17 Load Line Analysis  For a given V in : –Plot I dsn, I dsp vs. V out –V out must be where |currents| are equal in

CMOS VLSI DesignMOS equationsSlide 18 Load Line Analysis  V in = 0

CMOS VLSI DesignMOS equationsSlide 19 Load Line Analysis  V in = 0.2V DD

CMOS VLSI DesignMOS equationsSlide 20 Load Line Analysis  V in = 0.4V DD

CMOS VLSI DesignMOS equationsSlide 21 Load Line Analysis  V in = 0.6V DD

CMOS VLSI DesignMOS equationsSlide 22 Load Line Analysis  V in = 0.8V DD

CMOS VLSI DesignMOS equationsSlide 23 Load Line Analysis  V in = V DD

CMOS VLSI DesignMOS equationsSlide 24 Load Line Summary

CMOS VLSI DesignMOS equationsSlide 25 DC Transfer Curve  Transcribe points onto V in vs. V out plot

CMOS VLSI DesignMOS equationsSlide 26 Operating Regions  Revisit transistor operating regions RegionnMOSpMOS A B C D E

CMOS VLSI DesignMOS equationsSlide 27 Operating Regions  Revisit transistor operating regions RegionnMOSpMOS ACutoffLinear BSaturationLinear CSaturation DLinearSaturation ELinearCutoff

CMOS VLSI DesignMOS equationsSlide 28 Beta Ratio  If  p /  n  1, switching point will move from V DD /2  Called skewed gate  Other gates: collapse into equivalent inverter

CMOS VLSI DesignMOS equationsSlide 29 Noise Margins  How much noise can a gate input see before it does not recognize the input?

CMOS VLSI DesignMOS equationsSlide 30 Logic Levels  To maximize noise margins, select logic levels at

CMOS VLSI DesignMOS equationsSlide 31 Logic Levels  To maximize noise margins, select logic levels at –unity gain point of DC transfer characteristic

CMOS VLSI DesignMOS equationsSlide 32 Transient Response  DC analysis tells us V out if V in is constant  Transient analysis tells us V out (t) if V in (t) changes –Requires solving differential equations  Input is usually considered to be a step or ramp –From 0 to V DD or vice versa

CMOS VLSI DesignMOS equationsSlide 33 Inverter Step Response  Ex: find step response of inverter driving load cap

CMOS VLSI DesignMOS equationsSlide 34 Inverter Step Response  Ex: find step response of inverter driving load cap

CMOS VLSI DesignMOS equationsSlide 35 Inverter Step Response  Ex: find step response of inverter driving load cap

CMOS VLSI DesignMOS equationsSlide 36 Inverter Step Response  Ex: find step response of inverter driving load cap

CMOS VLSI DesignMOS equationsSlide 37 Inverter Step Response  Ex: find step response of inverter driving load cap

CMOS VLSI DesignMOS equationsSlide 38 Inverter Step Response  Ex: find step response of inverter driving load cap

CMOS VLSI DesignMOS equationsSlide 39 Delay Definitions  t pdr :  t pdf :  t pd :  t r :  t f : fall time

CMOS VLSI DesignMOS equationsSlide 40 Delay Definitions  t pdr : rising propagation delay –From input to rising output crossing V DD /2  t pdf : falling propagation delay –From input to falling output crossing V DD /2  t pd : average propagation delay –t pd = (t pdr + t pdf )/2  t r : rise time –From output crossing 0.2 V DD to 0.8 V DD  t f : fall time –From output crossing 0.8 V DD to 0.2 V DD

CMOS VLSI DesignMOS equationsSlide 41 Delay Definitions  t cdr : rising contamination delay –From input to rising output crossing V DD /2  t cdf : falling contamination delay –From input to falling output crossing V DD /2  t cd : average contamination delay –t pd = (t cdr + t cdf )/2

CMOS VLSI DesignMOS equationsSlide 42 Simulated Inverter Delay  Solving differential equations by hand is too hard  SPICE simulator solves the equations numerically –Uses more accurate I-V models too!  But simulations take time to write

CMOS VLSI DesignMOS equationsSlide 43 Delay Estimation  We would like to be able to easily estimate delay –Not as accurate as simulation –But easier to ask “What if?”  The step response usually looks like a 1 st order RC response with a decaying exponential.  Use RC delay models to estimate delay –C = total capacitance on output node –Use effective resistance R –So that t pd = RC  Characterize transistors by finding their effective R –Depends on average current as gate switches

CMOS VLSI DesignMOS equationsSlide 44 RC Delay Models  Use equivalent circuits for MOS transistors –Ideal switch + capacitance and ON resistance –Unit nMOS has resistance R, capacitance C –Unit pMOS has resistance 2R, capacitance C  Capacitance proportional to width  Resistance inversely proportional to width

CMOS VLSI DesignMOS equationsSlide 45 Example: 3-input NAND  Sketch a 3-input NAND with transistor widths chosen to achieve effective rise and fall resistances equal to a unit inverter (R).

CMOS VLSI DesignMOS equationsSlide 46 Example: 3-input NAND  Sketch a 3-input NAND with transistor widths chosen to achieve effective rise and fall resistances equal to a unit inverter (R).

CMOS VLSI DesignMOS equationsSlide 47 Example: 3-input NAND  Sketch a 3-input NAND with transistor widths chosen to achieve effective rise and fall resistances equal to a unit inverter (R).

CMOS VLSI DesignMOS equationsSlide 48 3-input NAND Caps  Annotate the 3-input NAND gate with gate and diffusion capacitance.

CMOS VLSI DesignMOS equationsSlide 49 3-input NAND Caps  Annotate the 3-input NAND gate with gate and diffusion capacitance.

CMOS VLSI DesignMOS equationsSlide 50 3-input NAND Caps  Annotate the 3-input NAND gate with gate and diffusion capacitance.

CMOS VLSI DesignMOS equationsSlide 51 Elmore Delay  ON transistors look like resistors  Pullup or pulldown network modeled as RC ladder  Elmore delay of RC ladder

CMOS VLSI DesignMOS equationsSlide 52 Example: 2-input NAND  Estimate worst-case rising and falling delay of 2- input NAND driving h identical gates.

CMOS VLSI DesignMOS equationsSlide 53 Example: 2-input NAND  Estimate rising and falling propagation delays of a 2- input NAND driving h identical gates.

CMOS VLSI DesignMOS equationsSlide 54 Example: 2-input NAND  Estimate rising and falling propagation delays of a 2- input NAND driving h identical gates.

CMOS VLSI DesignMOS equationsSlide 55 Example: 2-input NAND  Estimate rising and falling propagation delays of a 2- input NAND driving h identical gates.

CMOS VLSI DesignMOS equationsSlide 56 Example: 2-input NAND  Estimate rising and falling propagation delays of a 2- input NAND driving h identical gates.

CMOS VLSI DesignMOS equationsSlide 57 Example: 2-input NAND  Estimate rising and falling propagation delays of a 2- input NAND driving h identical gates.

CMOS VLSI DesignMOS equationsSlide 58 Example: 2-input NAND  Estimate rising and falling propagation delays of a 2- input NAND driving h identical gates.

CMOS VLSI DesignMOS equationsSlide 59 Delay Components  Delay has two parts –Parasitic delay 6 or 7 RC Independent of load –Effort delay 4h RC Proportional to load capacitance

CMOS VLSI DesignMOS equationsSlide 60 Contamination Delay  Best-case (contamination) delay can be substantially less than propagation delay.  Ex: If both inputs fall simultaneously

CMOS VLSI DesignMOS equationsSlide 61 Diffusion Capacitance  we assumed contacted diffusion on every s / d.  Good layout minimizes diffusion area  Ex: NAND3 layout shares one diffusion contact –Reduces output capacitance by 2C –Merged uncontacted diffusion might help too

CMOS VLSI DesignMOS equationsSlide 62 Layout Comparison  Which layout is better?