ECE 875: Electronic Devices

Slides:



Advertisements
Similar presentations
MICROWAVE FET Microwave FET : operates in the microwave frequencies
Advertisements

ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
EE105 Fall 2007Lecture 16, Slide 1Prof. Liu, UC Berkeley Lecture 16 OUTLINE MOS capacitor (cont’d) – Effect of channel-to-body bias – Small-signal capacitance.
Lecture 19 OUTLINE The MOSFET: Structure and operation
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices
Spencer/Ghausi, Introduction to Electronic Circuit Design, 1e, ©2003, Pearson Education, Inc. Chapter 2, slide 1 Introduction to Electronic Circuit Design.
ECE 874: Physical Electronics Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
MOS Capacitor Lecture #5. Transistor Voltage controlled switch or amplifier : control the output by the input to achieve switch or amplifier Two types.
The Devices: MOS Transistor
Chapter 6 The Field Effect Transistor
ECE 875: Electronic Devices
Electronics The Sixteenth and Seventh Lectures
ECE 875: Electronic Devices
Electronics The Fifteenth and Sixteenth Lectures
Lecture #14 OUTLINE Midterm #1 stats The pn Junction Diode
Recall Last Lecture Common collector Voltage gain and Current gain
GOVERMENT ENGINEERING COLLEGE
Revision CHAPTER 6.
Lecture 20 OUTLINE The MOSFET (cont’d) Qualitative theory
Lecture 22 OUTLINE The MOSFET (cont’d) MOSFET scaling
Intro to Semiconductors and p-n junction devices
Long Channel MOSFETs.
Electronics Chapter Four
EMT362: Microelectronic Fabrication CMOS ISOLATION TECHNOLOGY Part 1
Lecture 22 OUTLINE The MOSFET (cont’d) Velocity saturation
Long Channel MOS Transistors
Lecture 16 ANNOUNCEMENTS OUTLINE MOS capacitor (cont’d)
Lecture 19 OUTLINE The MOSFET: Structure and operation
Lecture 13: Part I: MOS Small-Signal Models
منبع: & کتابMICROELECTRONIC CIRCUITS 5/e Sedra/Smith
Reading: Finish Chapter 17,
ECE 874: Physical Electronics
ECE 875: Electronic Devices
Long Channel MOS Transistors
MOSFETs - An Introduction
ECE 874: Physical Electronics
Chapter 1 – Semiconductor Devices – Part 2
ECE 874: Physical Electronics
Chapter 2 – Transistors – Part 2
ECE 875: Electronic Devices
ECE 875: Electronic Devices
Lecture 3 OUTLINE Semiconductor Basics (cont’d) PN Junction Diodes
ECE 874: Physical Electronics
Lecture 20 OUTLINE The MOSFET (cont’d) Qualitative theory
EXAMPLE 7.1 BJECTIVE Determine the total bias current on an IC due to subthreshold current. Assume there are 107 n-channel transistors on a single chip,
Lecture 22 OUTLINE The MOSFET (cont’d) MOSFET scaling
ECE 875: Electronic Devices
Lecture 22 OUTLINE The MOSFET (cont’d) Velocity saturation
Lecture #15 OUTLINE Diode analysis and applications continued
ECE 875: Electronic Devices
ECE 875: Electronic Devices
Lecture 20 OUTLINE The MOSFET (cont’d)
ECE 875: Electronic Devices
Lecture 20 OUTLINE The MOSFET (cont’d)
ECE 875: Electronic Devices
ECE 875: Electronic Devices
ECE 875: Electronic Devices
Modern Semiconductor Devices for Integrated Circuits (C. Hu)
ELECTRONICS AND SOLID STATE DEVICES-II
ECE 875: Electronic Devices
Presentation transcript:

ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu

Lecture 32, 31 Mar 14 Chp 06: MOSFETs pn junctions/Depletion regions (examples) Channel Current IDS (n-channel p-substrate) VM Ayres, ECE875, S14

Chp. 04: MOS: Gate Chp. 03: Interconnect Chp. 01: Si Chp. 02: pn n-p-n VM Ayres, ECE875, S14

Qs ys ys For examples: VGate Si @ r.t. Substrate is p-type with NA = 4 x 1015 cm-3 Matches Fig. 4.5 Does not match Fig. 4.10 (b) Qs ys ys VGate VM Ayres, ECE875, S14

Example: What kind of pn junction is this: forward bias, reverse bias or equilibrium? VM Ayres, ECE875, S14

Answer: Equilibrium: earth to earth. Continue Example: Find WD VM Ayres, ECE875, S14

Answer: VM Ayres, ECE875, S14

Example: M-O-S depletion region is identified Example: M-O-S depletion region is identified. Find WDmax @ full inversion. + VG -  gnd VM Ayres, ECE875, S14

VM Ayres, ECE875, S14

WD = WDmax = WDm for low frequency operation VM Ayres, ECE875, S14

From Lec 31: Fig 4.8 (a): after strong inversion, increase Qm  increase Qn while QDep and therefore WD stay the same. Low frequency High frequency, Slow ramp High frequency, Fast ramp WDmax is bigger WDmax is biggest Qn layer; no time to form at all Qn smaller Qn biggest VM Ayres, ECE875, S14

n=channel p-substrate “knee” in Vfor  strong inversion. For VG less than value for strong inversion: Can find ys(VG) as in Pr. 4.05 using equivalent of Fig 4.10 (b). Note: this is Fgi. 10 (b). C-V in Fig. 4.10 (a) shows that this  low frequency operation. ys VGate Warning: Fig. 4.10 is for NA = 1 x 1016 cm-3 not our example! VM Ayres, ECE875, S14

Example: Is there an electric field across the channel region? Sub-question: “across” in which direction? + VG -  gnd + VDS -  gnd VM Ayres, ECE875, S14

First check coordinate system: Chp. 04: MOS: Gate Chp. 03: Interconnect Chp. 01: Si Chp. 02: pn n-p-n VM Ayres, ECE875, S14

First check coordinate system: Take “across”  Drain-Source: E (y)  “0” < y < length of channel L L z Width = Z y SiO2 x Width of gate/ charge sheet under gate in a MOSFET is called “Z”. It is a dimension in e.g., cm. Don’t confuse with atomic number. VM Ayres, ECE875, S14

Answer: Yes. There are (different) electric fields in both the y and x directions. + VG -  gnd + VDS -  gnd VM Ayres, ECE875, S14

E (y) is due to the potential drop across the channel: Answer: E (y) is due to the potential drop across the channel: e-’s move by F = q E (y) drift motion in the channel. + VG -  gnd + VDS -  gnd VM Ayres, ECE875, S14

Example: Is the shaded region an E (y) -field region or a pn junction depletion region? + VG -  gnd VM Ayres, ECE875, S14

Answer: Mixed. May have different field properties than channel. See Pr. 6.02. + VG -  gnd VM Ayres, ECE875, S14

Same here, see Pr. 02. + VG -  gnd VM Ayres, ECE875, S14

Note that Qn = Qn(y) in the Fig. + VG -  gnd + VDS -  gnd VM Ayres, ECE875, S14

Example: What kind of pn junction is this: forward bias, reverse bias or equilibrium? Assume VDS is on, as shown. + VG -  gnd + VDS -  gnd VM Ayres, ECE875, S14

Answer: Reverse bias. Continue Example: Find WD for Vrev = -6V. + VG -  gnd + VDS -  gnd VM Ayres, ECE875, S14

Answer: VM Ayres, ECE875, S14

Answer: Drain pn junction with VDS on Source pn junction with VDS on VM Ayres, ECE875, S14

The bigger depletion region at the Drain end leads to a physical pinch, which leads to saturation current. IDS  free Qn . Qn  Qn(y) VM Ayres, ECE875, S14

Lecture 32, 31 Mar 14 Chp 06: MOSFETs pn junctions/Depletion regions (examples) Channel Current IDS (n-channel p-substrate) VM Ayres, ECE875, S14

Channel current IDS Units-based guess: Need a length. Multiply by channel length L or channel width Z? ? VM Ayres, ECE875, S14

Channel current IDS Units-based guess: Need a length. Multiply by channel length L or channel width Z? ? Answer: IDS = Z Qn vel => dIDS = Z dQn(y) vel(y) some dy then IDS =Sum up (integrate) dIDS VM Ayres, ECE875, S14

Charge sheet model: to deal with Qn(y) Constant mobility model: to deal with vel(y) VM Ayres, ECE875, S14

Result of Charge sheet model: Result of constant mobility model: VM Ayres, ECE875, S14

Result of Charge sheet model: VM Ayres, ECE875, S14

Example: VM Ayres, ECE875, S14

Channel width Z changes, channel length L stays the same Therefore: You fabricated a new device with a different gate dimension. VM Ayres, ECE875, S14

Example: For the new device, Z = ? to do the specified job. VM Ayres, ECE875, S14

Answer: Given: device 01 is a “Square” MOSFET: Length L = width Z VM Ayres, ECE875, S14

Answer: Did not change the Drain or Gate batteries as well as the gate length VM Ayres, ECE875, S14

Answer: VM Ayres, ECE875, S14

Answer: Dividing info from two readings to get rid of common unknowns is a standard approach. VM Ayres, ECE875, S14