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NEMO5 Overview Presentation
17 Jul 2012 | | Contributor(s):: Tillmann Christoph Kubis, Michael Povolotskyi, Jean Michel D Sellier, James Fonseca, Gerhard Klimeck
This presentation gives an overview of the current functionality of NEMO5.
From Semi-Classical to Quantum Transport Modeling: What is Computational Electronics?
10 Aug 2009 | | Contributor(s):: Dragica Vasileska
This set of powerpoint slides series provides insight on what are the tools available for modeling devices that behave either classically or quantum-mechanically. An in-depth description is provided to the approaches with emphasis on the advantages and disadvantages of each approach. Conclusions...
From Semi-Classical to Quantum Transport Modeling: Drift-Diffusion and Hydrodynamic Modeling
From Semi-Classical to Quantum Transport Modeling: Particle-Based Device Simulations
From Semi-Classical to Quantum Transport Modeling: Quantum Corrections to Semiclassical Approaches
From Semi-Classical to Quantum Transport Modeling: Quantum Transport - Usuki Method and Theoretical Description of Green's Functions
From Semi-Classical to Quantum Transport Modeling: Quantum Transport - Recursive Green's function method, CBR approach and Atomistic
From Semi-Classical to Quantum Transport Modeling
ECE 659 Teaching Materials: Homeworks and Exams (Spring 2009)
24 Jun 2009 | | Contributor(s):: Supriyo Datta
Teaching materials for ECE 659 "Quantum Transport: Atom to Transistor".
OMEN Nanowire Demonstration: Nanowire Simulation and Analysis
11 Jun 2009 | | Contributor(s):: Gerhard Klimeck, Benjamin P Haley
This video shows the simulation and analysis of a nanowire using OMEN Nanowire. Several powerful analytic features of this tool are demonstrated.
ECE 659 Lecture 38.0: Correlations and Entanglement
04 May 2009 | | Contributor(s):: Supriyo Datta
This lecture is from the series of lecturesNanoelectronics and the Meaning of Resistance.
Thermoelectric Power Factor Calculator for Superlattices
18 Oct 2008 | | Contributor(s):: Terence Musho, Greg Walker
Quantum Simulation of the Seebeck Coefficient and Electrical Conductivity in 1D Superlattice Structures using Non-Equilibrium Green's Functions
Spins and Magnets (Whiteboard lecture), Part 1
out of 5 stars
06 Jan 2009 | | Contributor(s):: Supriyo Datta
Whiteboard version of approximately the same material covered in Lectures 3A/3B.
Spins and Magnets (Whiteboard lecture), Part 2
02 Sep 2008 | | Contributor(s):: SungGeun Kim, Mathieu Luisier, Benjamin P Haley, Abhijeet Paul, Saumitra Raj Mehrotra, Gerhard Klimeck, Hesameddin Ilatikhameneh
Full-band 3D quantum transport simulation in nanowire structure
Thermoelectric Power Factor Calculator for Nanocrystalline Composites
Quantum Simulation of the Seebeck Coefficient and Electrical Conductivity in a 2D Nanocrystalline Composite Structure using Non-Equilibrium Green's Functions
Quantum and Thermal Effects in Nanoscale Devices
18 Sep 2008 | | Contributor(s):: Dragica Vasileska
To investigate lattice heating within a Monte Carlo device simulation framework, we simultaneously solve the Boltzmann transport equation for the electrons, the 2D Poisson equation to get the self-consistent fields and the hydrodynamic equations for acoustic and optical phonons. The phonon...
Lecture 6: Quantum Transport in Nanoscale FETs
12 Sep 2008 | | Contributor(s):: Mark Lundstrom
The previous lessons developed an analytical (or almost analytical) theory of the nanoscale FET, but to properly treat all the details, rigorous computer simulations are necessary. This lecture presents quantum transport simulations that display the internal physics of nanoscale MOSFETs. We use...
Nanoelectronics and the meaning of resistance: Course Handout and Exercises
02 Sep 2008 | | Contributor(s):: Supriyo Datta
Handout with reference list, MATLAB scripts and exercise problems.
Lecture 4A: Energy Exchange and Maxwell's Demon
Objective: To incorporate distributed energy exchange processes into the previous models from lectures 1 through 3 which are based on a "Landauer-like picture" where the Joule heating associated with current flow occurs entirely in the two contacts.Although there is experimental evidence that...