-
ECE 606 L19.1: PN Junction - Structure and Depletion Region
Online Presentations | 20 Jul 2023 | Contributor(s):: Gerhard Klimeck
-
ECE 606 L24.2: Bipolar Junction Transistor - Band Diagram in Equilibrium
Online Presentations | 20 Jul 2023 | Contributor(s):: Gerhard Klimeck
-
ECE 606 L24.3: Bipolar Junction Transistor - Currents in BJTs
Online Presentations | 20 Jul 2023
-
ECE 606 L28.1: MOS Electrostatics and MOScap - Background
Online Presentations | 20 Jul 2023 | Contributor(s):: Gerhard Klimeck
-
ECE 606 L28.2: MOScap - Band Diagram in Equilibrium and with Bias -->MOS cap
Online Presentations | 20 Jul 2023 | Contributor(s):: Gerhard Klimeck
-
ECE 606 L28.5: MOScap - Exact Solution of the Electrostatic Problem
Online Presentations | 20 Jul 2023 | Contributor(s):: Gerhard Klimeck
-
ECE 606 L29.1: MOS Capacitor Signal Response - Introduction/Background
Online Presentations | 20 Jul 2023 | Contributor(s):: Gerhard Klimeck
-
ECE 595E Lecture 9: Programming for Linear Algebra
Online Presentations | 01 Feb 2013 | Contributor(s):: Peter Bermel
Outline:Recap from FridayApplication ExamplesElectrostatic potential (Poisson’s equation)1D array of charge2D grid of chargeArrays of interacting spins1D interaction along a chain2D nearest-neighbor coupling
-
ECE 606 Lecture 21: MOS Electrostatics
Online Presentations | 26 Nov 2012 | Contributor(s):: Gerhard Klimeck
-
ECE 606 Lecture 16: p-n Diode AC Response
Online Presentations | 24 Oct 2012 | Contributor(s):: Gerhard Klimeck
-
ECE 606 Lecture 15: p-n Diode Characteristics
Online Presentations | 17 Oct 2012 | Contributor(s):: Gerhard Klimeck
-
ECE 606 Lecture 14: p-n Junctions
Online Presentations | 04 Oct 2012 | Contributor(s):: Gerhard Klimeck
-
Nanoscale Transistors Lecture 4: MOS Electrostatics
Online Presentations | 19 Jul 2012 | Contributor(s):: Mark Lundstrom
-
Particle Simulations of Ion Generation and Transport in Microelectromechanical Systems and Micropropulsion
Online Presentations | 29 May 2012 | Contributor(s):: Venkattraman Ayyaswamy
The first part of the talk deals with use of the PIC method with Monte Carlo collisions (MCC) between electrons and the ambient neutral gas to develop models to predict charge accumulation, breakdown voltage, etc. for various ambient gases, gap sizes, cathode material, and frequency of applied...
-
2010 Nano-Biophotonics Summer School @ UIUC Lecture 2 - 2D/3D Fourier transforms & Electromagnetic fields/ Lorentz-Drude model
Online Presentations | 25 Sep 2010 | Contributor(s):: Gabriel Popescu
So far, we have discussed Fourier transformations involving one-dimensional functions. Of course, in studying imaging, the conceptmust be generalized to 2D and 3D functions. For example, diffraction and 2D image formation are treated efficiently via 2D Fouriertransforms, while light scattering...
-
ME 597 Lecture 25: Using the AFM to Measure Electrostatic Forces
Online Presentations | 02 Dec 2009 | Contributor(s):: Ron Reifenberger
-
Illinois ECE 440 Solid State Electronic Devices, Lecture 18: P-N Diode Electrostatics
Online Presentations | 22 Oct 2009 | Contributor(s):: Eric Pop
Last time, we talked about p-n junction built-in voltage V¬0.Today: more about p-n electrostatics.
-
ECE 606 Lecture 33: MOS Electrostatics II
Online Presentations | 16 Apr 2009 | Contributor(s):: Muhammad A. Alam
-
ECE 606 Lecture 20: Electrostatics of P-N Junction Diodes
Online Presentations | 11 Mar 2009 | Contributor(s):: Muhammad A. Alam
-
ECE 612 Lecture 25: SOI Electrostatics
Online Presentations | 08 Dec 2008 | Contributor(s):: Mark Lundstrom
Outline:1. Introduction,2. General solution, 3. VTF vs. VGB,4. Subthreshold slope,5. Double gate (DG) SOI,6. Recap,7. Discussion,8. Summary.