Device Models (PN Diode, MOSFET )


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1 Device Models (PN Diode, MOSFET ) Instructor: Steven P. Levitan TA: Gayatri Mehta, José Martínez Book: Digital Integrated Circuits: A Design Perspective; Jan Rabaey Lab Notes: Handed out ECE 1192, 2006, Steven Levitan, University of Pittsburgh
2 Goal of this chapter Present intuitive understanding of device operation Introduction of basic device equations Introduction of models for manual analysis Introduction of models for SPICE simulation Analysis of secondary and deepsubmicron effects Future trends
3 The DIODE B Al A SiO 2 p n Crosssection of pnjunction in an IC process A p n B Onedimensional representation Al A B diode symbol Mostly occurring as parasitic element in Digital ICs
4 Diodes in a CMOS circuit Copyright 2005 Pearson AddisonWesley. All rights reserved.
5 Depletion Region Formation hole diffusion electron diffusion p n (a) Current flow. hole drift electron drift Charge Density  ρ + x Distance (b) Charge density. Electrical Field ξ x (c) Electric field. Potential V ψ 0 W 1 W 2 x (d) Electrostatic potential.
6 Formation and characteristics of a pn junction Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
7 Forward Bias p n (W 2 ) p n0 L p n p0 pregion W 1 0 W 2 nregion x diffusion Typically avoided in Digital ICs
8 Reverse Bias p n0 n p0 pregion W 1 0 W 2 nregion x diffusion The Dominant Operation Mode
9 Diode Current a Simple Model
10 Models for Manual Analysis V D + I D = I S (e V D/φT 1) V D + + I D V Don (a) Ideal diode model (b) Firstorder diode model
11 PN Junction Diode DC Model (Details) Thermal Voltage Ф T = kt/q V ( 300 K) k Boltzmann constant ( x1023 J/K) T Absolute temperature ( K) q Electron charge ( x1019 C) I s In practice, this term has to be obtained by characterization since it is highly dependent on doping concentration, dimension, operative temperature etc. ECE , Steven Levitan, University of Pittsburgh
12 PN Junction: Dynamic Effects Primary effects Junction Capacitance Diffusion Capacitance Secondary Effects Avalanche Breakdown ECE , Steven Levitan, University of Pittsburgh
13 Junction Capacitance
14 Diffusion Capacitance
15 Integrated Diode Model R S + V D  I D C D
16 SPICE Parameters
17 The MOS Transistor Polysilicon Aluminum
18 Controlling current flow in an nfet. Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
19 Controlling current flow in an pfet. Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
20 What is a Transistor? A Switch! An MOS Transistor V GS V T V GS S Ron D
21 MOS Transistors  Types and Symbols D D G G S NMOS Enhancement D S NMOS Depletion D G G B PMOS Enhancement S S NMOS with Bulk Contact
22 MOS Transistors Regions Transitions Copyright 2005 Pearson AddisonWesley. All rights reserved.
23 Threshold Voltage: Concept S  V GS + G D n+ n+ nchannel psubstrate Depletion Region B
24 Threshold Voltage  Derivation
25 The Body Effect input NAND gate V DD 0.75 V T (V) V (V) BS B A N2 N1 Drain of N1 is Source of N2 VSB of N2 >= 0
26 MOS Transistors Operating regions Copyright 2005 Pearson AddisonWesley. All rights reserved.
27 Transistor in Linear S V GS G V DS D I D n + V(x) + n + L x psubstrate B MOS transistor and its bias conditions
28 Linear Region Vgs>V t & Vgd>V t S V GS G V DS D I D I ds n + V(x) + n + V gd L psubstrate x V gs R Positive Charge on Gate: Channel exists, Current Flows since V ds > 0 I ds = k (W/L)((V gs V t )V ds V ds2 /2) B I ds I=V/R R= 1/(k (W/L)(V gs V t )) V ds
29 Transistor in Saturation V GS G V DS > V GS  V T S D n+  V GS  V T + n+ Pinchoff
30 Saturation: Vgs>V t & Vgd<V t V GS I ds G V DS > V GS  V T V gd S D I ds n+  V GS  V T + n+ V gs Positive Charge on Gate: Channel exists, Current Flows since V ds > 0 But: channel is pinched off I ds = (k /2)(W/L)(V gs V t ) 2
31 CurrentVoltage Relations A good ol transistor 4 x 10 6 VGS= 2.5 V 5 4 Resistive Saturation VGS= 2.0 V I D (A) 3 V DS = V GS V T Quadratic Relationship 2 VGS= 1.5 V 1 VGS= 1.0 V V DS (V)
32 CurrentVoltage Relations LongChannel Device Cutoff (V GS V T < 0) no current (not really)
33 Computed Curves Linear Resistor Vgs = 5v Vgs = 4.5v Vgs = 4.0v
34 CurrentVoltage Relations The DeepSubmicron Era 2.5 x Early Saturation VGS= 2.5 V 1.5 VGS= 2.0 V I D (A) 1 VGS= 1.5 V Linear Relationship 0.5 VGS= 1.0 V V DS (V)
35 Velocity Saturation υ n (m/s) υ sat = 10 5 Constant velocity Constant mobility (slope = µ) ξ c = 1.5 ξ (V/µm)
36 Perspective I D Longchannel device V GS = V DD Shortchannel device V DSAT V GS V T V DS
37 I D versus V GS 6 x x quadratic linear I D (A) 3 I D (A) V GS (V) Long Channel 0.5 quadratic V GS (V) Short Channel
38 I D versus V DS I D (A) 6 x VGS= 2.5 V Resistive Saturation VGS= 2.0 V V DS = V GS V T VGS= 1.5 V I D (A) x 10 VGS= 2.5 V VGS= 2.0 V VGS= 1.5 V 1 VGS= 1.0 V 0.5 VGS= 1.0 V V DS (V) Long Channel V DS (V) Short Channel
39 A unified model for manual analysis G S D B
40 Simple Model versus SPICE 2.5 x 104 V DS =V DSAT Velocity Saturated I D (A) 1 Linear 0.5 V DSAT =V GT V DS =V GT Saturated V DS (V)
41 A PMOS Transistor 0 x 104 VGS = 1.0V 0.2 VGS = 1.5V 0.4 I D (A) 0.6 VGS = 2.0V Assume all variables negative! 0.8 VGS = 2.5V V DS (V)
42 Transistor Model for Manual Analysis
43 The Transistor as a Switch V GS V T S Ron I D D V GS = V DD R mid R 0 V DD /2 V DD V DS
44 The Transistor as a Switch 7 x R eq (Ohm) V DD (V)
45 The Transistor as a Switch
46 Saturation Effects Discharge of 1pf capacitor, with Vgs of 3,4,5 volts. Also, 12k resistor. Which is the resistor?
47 MOS Capacitances Dynamic Behavior
48 Dynamic Behavior of MOS Transistor G C GS C GD S D C SB C GB C DB B
49 Physical visualization of FET capacitances Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
50 MOS Capacitances Behavior! Copyright 2005 Pearson AddisonWesley. All rights reserved.
51 The Gate Capacitance in an nchannel n MOSFET Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
52 The Gate Capacitance Polysilicon gate Source n + x d x d W Drain n + L d Top view Gatebulk overlap t ox Gate oxide n + L n + Cross section
53 Gate Capacitance Copyright 2005 Pearson AddisonWesley. All rights reserved.
54 Gate Capacitance Behavior G G G S C GC C GC C GC D S D S D Cutoff Resistive Saturation Most important regions in digital design: saturation and cutoff
55 Gate Capacitance Behavior WLC ox C GC WLC ox C GC 2WLC ox WLC ox 2 C GC B C GCS = C GCD WLC ox 2 C GCS C GCD 3 V GS 0 V DS /(V GS V T ) 1 Capacitance as a function of VGS (with VDS = 0) Capacitance as a function of the degree of saturation
56 Measuring the Gate Cap I V GS Gate Capacitance (F) V GS (V)
57 Diffusion Capacitance Channelstop implant N A 1 Side wall W Source N D Bottom x j L S Side wall Substrate N A Channel
58 Junction capacitances in a MOSFET Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
59 Calculation of the FET junction capacitance Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
60 Junction capacitance variation with reverse voltage Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
61 Final construction of the nfet RC model C G Digital Integrated Circuits 2nd Introduction to Circuits, Fourth Edition by Peter Uyemura, Devices Copyright 2004 John Wiley & Sons. All rights reserved.
62 Capacitances in 0.25 μm m CMOS process Values for a Typical Device:
63 The SubMicron MOS Transistor Threshold Variations Subthreshold Conduction Parasitic Resistances
64 Threshold Variations V T V T Longchannel threshold Low V DS threshold Threshold as a function of the length (for low V DS ) L V DS Draininduced barrier lowering (for low L)
65 SubThreshold I D vs VGS qvgs nkt I D I0e 1 e qv = kt DS Log Scale V DS from 0 to 0.5V
66 SubThreshold I D vs VDS I D qvgs qv = nkt kt I e 0 1 e DS ( 1+ λ V ) DS V GS from 0 to 0.3V Linear scale
67 Summary of MOSFET Operating Regions Strong Inversion V GS >V T Linear (Resistive) V DS <V DSAT Saturated (Constant Current) V DS V DSAT Weak Inversion (SubThreshold) V GS V T Exponential in V GS with linear V DS dependence
68 Parasitic Resistances G Polysilicon gate L D Drain contact V GS,eff S D W R S R D Drain
69 Latchup V DD V DD p + n + n + p + p + n + R nwell psource nwell R nwell R psubs psubstrate nsource R psubs (a) Origin of latchup (b) Equivalent circuit
70 SPICE MODELS Level 1: Long Channel Equations  Very Simple Level 2: Physical Model  Includes Velocity Saturation and Threshold Variations Level 3: SemiEmperical  Based on curve fitting to measured devices Level 4 (BSIM): Emperical  Simple and Popular
71 Main MOS SPICE Parameters
72 SPICE Parameters for Parasitics
73 SPICE Transistors Parameters
74 Circuit Simulation Model of CMOS Inverter
Device Models (PN Diode, MOSFET )
Device Models (PN Diode, MOSFET ) Instructor: Steven P. Levitan steve@ece.pitt.edu TA: Gayatri Mehta, José Martínez Book: Digital Integrated Circuits: A Design Perspective; Jan Rabaey Lab Notes: Handed
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