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  1. ECE 695A Lecture 14b: Voltage Dependent HCI II

    19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam

    Outline:Background and Empirical ObservationsTheory of Hot Carriers: Hydrodynamic ModelTheory of Hot Carriers: Monte Carlo ModelTheory of Hot Carriers: Universal ScalingConclusionAppendices

  2. ECE 695A Lecture 14R: Review Questions

    19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam

    Review QuestionsWhy is Isub called a thermometer of hot electron distribution? Why can you not simply measure hot electrons by looking at the drain current?What are the three methods of HCI voltage acceleration?If theory of universal scaling is so good, why not use it all the time? (Hint: Think...

  3. ECE 595E Lecture 16: Applications of the Beam Propagation Method I

    21 Feb 2013 | Online Presentations | Contributor(s): Peter Bermel

  4. Optical Absorption in B13 Cluster: A Time-dependent Density Functional Approach

    19 Feb 2013 | Papers | Contributor(s): Ravindra L Shinde, Meenakshi Tayade

    The linear optical absorption spectra of three isomers of planar boron cluster B13 are calculated using time dependent spin-polarized density functional approach. The geometries of these cluster are optimized at the B3LYP/6-311+G* level of theory. Even though the isomers are almost degenerate,...

  5. ECE 695A Lecture 15: Off-state HCI Degradation

    19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam

    Outline:ON vs. OFF State HCI DegradationOrigin of hot carriers at off-stateSiH vs. SiO – who is getting broken? Voltage acceleration factors by scalingConclusions

  6. ECE 695A Lecture 16: Temperature Dependence of HCI

    19 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam

    Outline:Empirical observations regarding HCITheory of bond dissociation: MVE vs. RRKHot carrier dissociation of SiH bondsHot carrier dissociation of SiO bondsConclusions

  7. ECE 695A Lecture 15R: Review Questions

    20 Feb 2013 | Online Presentations | Contributor(s): Muhammad Alam

    Review Questions:Why is BTBT tunneling important for OFF-state HCI, but nor for ON-state HCI?What type of bond dissociation dominated DeMOS degradation? Provide two supporting arguments. Will universality hold of SiH and SiO bond dissociation occur in equal proportion?Do you expect NBTI to be...

  8. [Illinois] PHYS466 2013 Lecture 8: Correlations I

    06 Mar 2013 | Online Presentations | Contributor(s): David M. Ceperley, George Daley

    Professor Ceperley received his BS in physics from the University of Michigan in 1971 and his Ph.D. in physics from Cornell University in 1976. After one year at the University of Paris and a second postdoc at Rutgers University, he worked as a staff scientist at both Lawrence Berkeley and...

  9. Inelastic Transport in Carbon Nanotube Electronic and Optoelectronic Devices

    28 Jun 2013 | Papers | Contributor(s): Siyu Koswatta

    Discovered in the early 1990's, carbon nanotubes (CNTs) are found to have exceptional physical characteristics compared to conventional semiconductor materials, with much potential for devices surpassing the performance of present-day electronics. Semiconducting CNTs have large carrier...

  10. [Illinois] PHYS466 2013 Lecture 9: Correlations II

    08 Mar 2013 | Online Presentations | Contributor(s): David M. Ceperley

    Professor Ceperley received his BS in physics from the University of Michigan in 1971 and his Ph.D. in physics from Cornell University in 1976. After one year at the University of Paris and a second postdoc at Rutgers University, he worked as a staff scientist at both Lawrence Berkeley and...

  11. [Illinois] PHYS466 2013 Lecture 10: Dynamics

    06 Mar 2013 | Online Presentations | Contributor(s): David M. Ceperley

    Professor Ceperley received his BS in physics from the University of Michigan in 1971 and his Ph.D. in physics from Cornell University in 1976. After one year at the University of Paris and a second postdoc at Rutgers University, he worked as a staff scientist at both Lawrence Berkeley and...

  12. [Illinois] PHYS466 2013 Lecture 12: Constraints

    08 Mar 2013 | Online Presentations | Contributor(s): David M. Ceperley

    Professor Ceperley received his BS in physics from the University of Michigan in 1971 and his Ph.D. in physics from Cornell University in 1976. After one year at the University of Paris and a second postdoc at Rutgers University, he worked as a staff scientist at both Lawrence Berkeley and...

  13. [Illinois] PHYS466 2013 Lecture 13: Random Number Generators

    08 Mar 2013 | Online Presentations | Contributor(s): David M. Ceperley

    Professor Ceperley received his BS in physics from the University of Michigan in 1971 and his Ph.D. in physics from Cornell University in 1976. After one year at the University of Paris and a second postdoc at Rutgers University, he worked as a staff scientist at both Lawrence Berkeley and...

  14. [Illinois] ECE 416 Bio Structure/Function II + Mass Transport I

    26 Feb 2013 | Online Presentations | Contributor(s): Brian Cunningham

               In this lecture, the roles of antibodies and their structures are elaborated on from the last lecture. Then, there is a revision of DNA and RNA: the structure, the base pairs, the different nucleotides and the hydrogen bonds'...

  15. [Illinois] ECE 416 Assay Formats

    26 Feb 2013 | Online Presentations | Contributor(s): Brian Cunningham

               In this lecture, assays, which is the most widely used technique to detect molecules on surfaces are discussed. In the direct assays, there is a "labeled assay" method and a "label-Free Assay" method. The Label-Free Assay method...

  16. [Illinois]: Big Mess

    26 Jun 2013 | Tools | Contributor(s): Bara Saadah

    This tool stimulates the pulse or step response of a neural network with ten input and ten output units that are randomly connected.

  17. [Illinois] ECE 416 Mass Transport II

    26 Feb 2013 | Online Presentations | Contributor(s): Brian Cunningham

               In this lecture, we look at the mass transfer coefficient of association and dissociation rates of molecules on the biosensor and off of it. Having a flow cell speeds it up, but the molecules must get through a stagnant layer to...

  18. [Illinois] ECE 416 Electrochemical Sensors

    27 Feb 2013 | Online Presentations | Contributor(s): Brian Cunningham

               In this lecture, we begin discussing the three types of electrochemical sensors: Potentiometric, Amperometric, and Conductometry. The focus of the lecture is the potentiometric and how it is used to measure the potential...

  19. [Illinois] ECE 416 Glucose Sensor I

    27 Feb 2013 | Online Presentations | Contributor(s): Brian Cunningham

               In this lecture, we continue the discussion on the oxygen sensor. It starts with a review of the measurement of O2 concentration levels through electrical currents. This is called an amperometric meter. Then, the subject shifts to...

  20. [Illinois]: Sigmoidal unit training with the delta rule

    26 Jun 2013 | Tools | Contributor(s): Lisa Sproat, NanoBio Node, Jessica S Johnson

    Uses the delta rule to train a single sigmoidal unit with feedback to simulate the responses of neurons in the parabigeminal nucleus

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