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  1. ECE 595Z Lecture 7: Two-level Logic Synthesis II

    27 Aug 2012 | Online Presentations | Contributor(s): Anand Raghunathan

  2. ECE 595Z Lecture 8: Two-level Logic Synthesis III

    27 Aug 2012 | Online Presentations | Contributor(s): Anand Raghunathan

  3. ECE 595Z Lecture 9: Two-level Logic Synthesis IV

    27 Aug 2012 | Online Presentations | Contributor(s): Anand Raghunathan

  4. ECE 595Z Lecture 13: Boolean Satisfiability III

    30 Aug 2012 | Online Presentations | Contributor(s): Anand Raghunathan

  5. ECE 595Z Lecture 11: Boolean Satisfiability I

    30 Aug 2012 | Online Presentations | Contributor(s): Anand Raghunathan

  6. ECE 595Z Lecture 12: Boolean Satisfiability II

    30 Aug 2012 | Online Presentations | Contributor(s): Anand Raghunathan

  7. Near-field radiation transport between two planes

    28 Aug 2012 | Tools | Contributor(s): Majid alDosari, Greg Walker

    Calculates the radiation exchange between two parallel half-spaces

  8. ECE 606 Solid State Devices

    10 Oct 2012 | Courses | Contributor(s): Gerhard Klimeck

  9. ECE 606 Lecture 1: Introduction/Crystal Classification

    30 Aug 2012 | Online Presentations | Contributor(s): Gerhard Klimeck

  10. MSE 597GM Lecture 4: Losses in Battery Materials

    13 Sep 2012 | Online Presentations | Contributor(s): R. Edwin García

  11. ECE 606 Lecture 2: Quantum Mechanics

    14 Sep 2012 | Online Presentations | Contributor(s): Gerhard Klimeck

  12. ECE 606 Lecture 3: Emergence of Bandstructure

    31 Aug 2012 | Online Presentations | Contributor(s): Gerhard Klimeck

    Table of Contents:00:00ECE606: Solid State Devices Lecture 300:24Motivation01:17Time-independent Schrodinger Equation02:22Time-independent Schrodinger Equation04:23A Simple Differential Equation05:29Presentation Outline05:46Full Problem Difficult: Toy Problems First06:07Case 1: Solution for...

  13. MSE 597GM Lecture 5: The Reaction Zone Model I

    13 Sep 2012 | Online Presentations | Contributor(s): R. Edwin García

  14. ECE 606 Lecture 4: Periodic Potentials Solutions of Schrödinger's Equation

    14 Sep 2012 | Online Presentations | Contributor(s): Gerhard Klimeck

  15. A CNTFET-Based Nanowired Induction Two-Way Transducers

    05 Sep 2012 | Papers | Contributor(s): Rostyslav Sklyar

    A complex of the induction magnetic field two-way nanotransducers of the different physical values for both the external and implantable interfaces in a wide range of arrays are summarized. Implementation of the nanowires allows reliable transducing of the biosignals' partials and bringing of...

  16. Optical absorption in boron clusters B6 and B6+ : A first principles configuration interaction approach

    07 Sep 2012 | Papers | Contributor(s): Ravindra L Shinde

    The linear optical absorption spectra in neutral boron cluster B6 and cationic B6+ are calculated using a first principles correlated electron approach. The geometries of several low-lying isomers of these clusters were optimized at the coupled-cluster singles doubles (CCSD) level of theory....

  17. DBR Laser Simulator

    07 Sep 2012 | Tools | Contributor(s): Nikhil Sancheti, Lynford Goddard, Christopher Adam Edwards

    Describes properties of a GaAs/AlGaAs DBR laser

  18. MSE 597GM Lecture 6: The Reaction Zone Model II

    13 Sep 2012 | Online Presentations | Contributor(s): R. Edwin García

  19. S4: Stanford Stratified Structure Solver

    11 Sep 2012 | Tools | Contributor(s): Jiarui Kang, Xufeng Wang, Peter Bermel, Chang Liu

    S4 is a frequency domain code to solve layered periodic structures. Internally, it uses Rigorous Coupled Wave Analysis (RCWA; also called the Fourier Modal Method (FMM)) and the S-matrix algorithm.

  20. Tight Binding Parameters by DFT mapping

    12 Sep 2012 | Presentation Materials | Contributor(s): Yaohua Tan, Michael Povolotskyi, Tillmann Christoph Kubis, Yu He, Zhengping Jiang, Gerhard Klimeck, Timothy Boykin

    The Empirical Tight Binding(ETB) method is widely used in atomistic device simulations. The reliability of such simulations depends very strongly on the choice of basis sets and the ETB parameters. The traditional way of obtaining the ETB parameters is by fitting to experiment data,or critical...

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