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Tutorial 4c: Formation of Bandstructure in Finite Superlattices (Exercise Session)
Online Presentations | 29 Mar 2011 | Contributor(s):: Gerhard Klimeck
How does bandstructure occur? How large does a repeated system have to be? How does a finite superlattice compare to an infinite superlattice?
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Tutorial 4d: Formation of Bandstructure in Finite Superlattices (Exercise Demo)
Online Presentations | 29 Mar 2011 | Contributor(s):: Gerhard Klimeck
Demonstration of thePiece-Wise Constant Potential Barriers Tool.
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Atomistic Modeling and Simulation Tools for Nanoelectronics and their Deployment on nanoHUB.org
Online Presentations | 16 Dec 2010 | Contributor(s):: Gerhard Klimeck
At the nanometer scale the concepts of device and material meet and a new device is a new material and vice versa. While atomistic device representations are novel to device physicists, the semiconductor materials modeling community usually treats infinitely periodic structures. Two electronic...
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Discussion Session 2 (Lectures 3 and 4)
Online Presentations | 08 Sep 2010 | Contributor(s):: Supriyo Datta
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Lecture 3: Introduction to NEGF
Online Presentations | 08 Sep 2010 | Contributor(s):: Supriyo Datta
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Lecture 2: Quantum of Conductance: Resistance and uncertainty
Online Presentations | 08 Sep 2010
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Nanoelectronic Modeling Lecture 41: Full-Band and Atomistic Simulation of Realistic 40nm InAs HEMT
Online Presentations | 05 Aug 2010 | Contributor(s):: Gerhard Klimeck, Neerav Kharche, Neophytos Neophytou, Mathieu Luisier
This presentation demonstrates the OMEN capabilities to perform a multi-scale simulation of advanced InAs-based high mobility transistors.Learning Objectives:Quantum Transport Simulator Full-Band and Atomistic III-V HEMTs Performance Analysis Good Agreement with Experiment Some Open Issues...
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Lecture 1b: Nanotransistors - A Bottom Up View
Online Presentations | 20 Jul 2010 | Contributor(s):: Mark Lundstrom
MOSFET scaling continues to take transistors to smaller and smaller dimensions. Today, the MOSFET is a true nanoelectronic device – one of enormous importance for computing, data storage, and for communications. In this lecture, I will present a simple, physical model for the nanoscale...
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Nanoelectronic Modeling Lecture 25b: NEMO1D - Hole Bandstructure in Quantum Wells and Hole Transport in RTDs
Online Presentations | 09 Mar 2010 | Contributor(s):: Gerhard Klimeck
Heterostructures such as resonant tunneling diodes, quantum well photodetectors and lasers, and cascade lasers break the symmetry of the crystalline lattice. Such break in lattice symmetry causes a strong interaction of heavy-, light- and split-off hole bands. The bandstructure of holes and the...
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ECE 606 Lecture 38: Modern MOSFET
Online Presentations | 07 May 2009 | Contributor(s):: Muhammad A. Alam
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ECE 659 Lecture 38: Singlet/Triplet States I
Online Presentations | 06 May 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 39: Singlet/Triplet States II
Online Presentations | 06 May 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 40: Correlated Transport
Online Presentations | 06 May 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 41: Exchange Interaction
Online Presentations | 05 May 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 42: Summing Up
Online Presentations | 04 May 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 38.0: Correlations and Entanglement
Online Presentations | 04 May 2009 | Contributor(s):: Supriyo Datta
This lecture is from the series of lecturesNanoelectronics and the Meaning of Resistance.
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ECE 659 Lecture 37: Inelastic Transport
Online Presentations | 01 May 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 36: Law of Equilibrium
Online Presentations | 01 May 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 35: Entropy
Online Presentations | 28 Apr 2009 | Contributor(s):: Supriyo Datta
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ECE 659 Lecture 32: Spin Torque/Psuedo-Spin
Online Presentations | 16 Apr 2009 | Contributor(s):: Supriyo Datta