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  1. ECE 595Z Lecture 6: Two-level Logic Synthesis I

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

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

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

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

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

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

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

  5. ECE 595Z Lecture 13: Boolean Satisfiability III

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

  6. ECE 595Z Lecture 11: Boolean Satisfiability I

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

  7. ECE 595Z Lecture 12: Boolean Satisfiability II

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

  8. ECE 606 Lecture 1: Introduction/Crystal Classification

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

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

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

  10. ECE 606 Lecture 2: Quantum Mechanics

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

  11. 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...

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

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

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

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

  14. 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...

  15. 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....

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

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

  17. 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...

  18. MSE 597GM Lecture 7: Introduction to VKML

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

  19. MSE 597GM Lecture 8: VKML Tutorial/Python Crash Course

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

  20. 1-D Green's Functions For Heat Conduction Between Semi-infinite Slabs With Perfect and Imperfect Boundary Contact

    17 Jan 2013 | Papers | Contributor(s): Donald E. Amos

    This document presents two derivations for 1-D Green's functionsfor semi-infinite slabs in contact along the boundary x=0. The case ofimperfect contact with a heat transfer coefficient h is derived and the caseof perfect contact is obtained by taking h to infinity. The two dimensionalcase with...

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