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2010 Nano-Biophotonics Summer School @ UIUC Lecture 2 - 2D/3D Fourier transforms & Electromagnetic fields/ Lorentz-Drude model
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...
ABACUS - Assembly of Basic Applications for Coordinated Understanding of Semiconductors
16 Jul 2008 | | Contributor(s):: Xufeng Wang, Dragica Vasileska, Gerhard Klimeck
One-stop-shop for teaching semiconductor device education
Capacitance Modeling Tool Using Schwarz-Christoffel Mapping
20 Oct 2010 | | Contributor(s):: Fengyuan (Thomas) Li, jason clark
Calculate the capacitance between two conductors that may be represented as simply-connected polygonal geometries in 2.5D with Dirichlet boundary conditions
Carbon Nanotube Electronics: Modeling, Physics, and Applications
27 Jun 2013 | | Contributor(s):: Jing Guo
In recent years, significant progress in understanding the physics of carbon nanotube electronic devices and in identifying potential applications has occurred. In a nanotube, low bias transport can be nearly ballistic across distances of several hundred nanometers. Deposition of high-k gate...
Comb Drive Levitation
19 Jan 2010 | | Contributor(s):: Fengyuan (Thomas) Li, jason clark
Model comb drive levitation effect with Schwarz-Christoffel based algorithm
ECE 495N Lecture 3: Importance of Electrostatics
out of 5 stars
10 Sep 2008 | | Contributor(s):: Supriyo Datta
ECE 495N Lecture 5: Quantitative Model for Nanodevices II
12 Sep 2008 | | Contributor(s):: Supriyo Datta
ECE 595E Lecture 9: Programming for Linear Algebra
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 14: p-n Junctions
04 Oct 2012 | | Contributor(s):: Gerhard Klimeck
ECE 606 Lecture 15: p-n Diode Characteristics
17 Oct 2012 | | Contributor(s):: Gerhard Klimeck
ECE 606 Lecture 16: p-n Diode AC Response
24 Oct 2012 | | Contributor(s):: Gerhard Klimeck
ECE 606 Lecture 20: Electrostatics of P-N Junction Diodes
11 Mar 2009 | | Contributor(s):: Muhammad A. Alam
ECE 606 Lecture 21: MOS Electrostatics
26 Nov 2012 | | Contributor(s):: Gerhard Klimeck
ECE 606 Lecture 32: MOS Electrostatics I
19 Nov 2008 | | Contributor(s):: Muhammad A. Alam
ECE 606 Lecture 33: MOS Electrostatics II
16 Apr 2009 | | Contributor(s):: Muhammad A. Alam
ECE 612 Lecture 12: 2D Electrostatics
28 Oct 2008 | | Contributor(s):: Mark Lundstrom
Outline:1) Consequences of 2D electrostatics,2) 2D Poisson equation,3) Charge sharing model,4) Barrier lowering,5) 2D capacitor model,6) Geometric screening length,7) Discussion,8) Summary.
ECE 612 Lecture 14: VT Engineering
Outline: 1) VT Specification,2) Uniform Doping,3) Delta-function doping, xC = 0,4) Delta-function doping, xC > 0,5) Stepwise uniform,6) Integral solution.The doping profiles in modern MOSFETs are complex. Our goal is to develop an intuitive understanding of how non-uniform doping profiles affect...
ECE 612 Lecture 1: 1D MOS Electrostatics I
09 Sep 2008 | | Contributor(s):: Mark Lundstrom
Outline: 1) Review of some fundamentals,2) Identify next steps.
ECE 612 Lecture 25: SOI Electrostatics
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.
ECE 612 Lecture 2: 1D MOS Electrostatics II
Outline: 1) Review,2) ‘Exact’ solution (bulk), 3) Approximate solution (bulk), 4) Approximate solution (ultra-thin body), 5) Summary.