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nanoHUB - Educational Tour de Force
14 Jan 2016 | Online Presentations | Contributor(s): David K. Ferry
nanoHUB was originally created to bring together the computational electronics world as a place where programs and results could be efficiently shared. For that purpose, it has matured and grown to where it is a major force in the area. But, it can also be a great tool for education, an...
Using NanoHub in Undergraduate Education
25 Jun 2014 | Online Presentations | Contributor(s): David K. Ferry
nanoHUB.org has now been with us for quite some time. It has developed a suite of software simulation tools that is used extensively throughout the research community around the world. Some years back, I was tasked to find a way to create a laboratory for our course on “Electronic Materials and...
2D Scattering Rates Calculation
20 Jul 2010 | Teaching Materials | Contributor(s): Dragica Vasileska, David K. Ferry
this set of slides describes the calculation of the 2D scattering rates in Q2DEG.
Time-Dependent Perturbation Theory
20 Jul 2010 | Teaching Materials | Contributor(s): David K. Ferry, Dragica Vasileska
This set of slides describes in detail the derivation of Fermi's Golden Rule.
This set of slides describes the derivation of Fermi-Dirac, Maxwell-Boltzmann and Bose-Einstein statistics.
Explanation of Rode's Iterative Procedure
This set of slides describes the Rode's iterative procedure for the mobility calculation when the scattering mechanisms are neither elastic nor isotropic such as is polar optical phonon scattering.
Crystal Directions and Miller Indices
08 Jun 2010 | Teaching Materials | Contributor(s): David K. Ferry, Dragica Vasileska, Gerhard Klimeck
Miller indices are a notation system in crystallography for planes and directions in crystal lattices. In particular, a family of lattice planes is determined by three integers, l, m, and n, the Miller indices. They are written (lmn) and denote planes orthogonal to a direction (l,m,n) in the...
In mineralogy and crystallography, a crystal structure is a unique arrangement of atoms in a crystal. A crystal structure is composed of a basis, a set of atoms arranged in a particular way, and a lattice. The basis is located upon the points of a lattice spanned by lattice vectors, which is an...
Slides: Time-Dependent Perturbation Theory
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10 Jul 2008 | Teaching Materials | Contributor(s): Dragica Vasileska, David K. Ferry
Slides: Examples and Stark Effect
Slides: Degenerate Perturbation Theory
Slides: Stationary Perturbation Theory
Slides: WKB Approximation 2
09 Jul 2008 | Teaching Materials | Contributor(s): Dragica Vasileska, David K. Ferry
Slides: WKB Approximation 1
Harmonic Oscillator: Motion in a Magnetic Field
Slides: Harmonic Oscillator - Operator Approach
Slides: Harmonic Oscillator - Brute Force Approach
Quantum Mechanics for Engineers: Podcasts
07 Jul 2008 | Series | Contributor(s): Dragica Vasileska, Gerhard Klimeck, David K. Ferry
This course will introduce the students to the basic concepts and postulates of quantum mechanics. Examples will include simple systems such as particle in an infinite and finite well, 1D and 2D harmonic oscillator and tunneling. Numerous approximation techniques, such as WKB method,...
Slides on Introductory Concepts in Quantum Mechanics
07 Jul 2008 | Teaching Materials | Contributor(s): Dragica Vasileska, David K. Ferry, Gerhard Klimeck
particle wave duality, quantization of energy
Quantum Mechanics: Introductory Concepts
In this section of the Quantum Mechanics class we discuss the particle-wave duality and the need for the quantization of energy to explain the black-body radiation and the photoelectric effect. We provide reading material, slides and video, which in a very illustrative way, explain the most...
Ensemble Monte Carlo Method Described
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27 Apr 2008 | Online Presentations | Contributor(s): Dragica Vasileska, Gerhard Klimeck, Mark Lundstrom, David K. Ferry
In this presentation we give an overview of the implementation details of the Ensemble Monte Carlo method for mobility and drift velocity calculation in arbitrary materials and arbitrary crystalographic orientations.NSF-Career, ONR
Modeling Coulomb Effects in Nanoscale Devices
26 Apr 2008 | Online Presentations | Contributor(s): Dragica Vasileska, Shaikh S. Ahmed, David K. Ferry
We describe the development of the modeling efforts focused towards proper description of the threshold voltage fluctuations due to the discrete impurity effects (different number and different distribution of the impurities from device to device on the same chip).NSF, ONRW. J. Gross, D....
Homework Assignment: Periodic Potentials
31 Jan 2008 | Teaching Materials | Contributor(s): David K. Ferry
Using the Periodic Potential Lab on nanoHUB determine the allowed bands for an energy barrier of 5 eV, a periodicity W = 0.5nm, and a barrier thickness of 0.1nm. How do these bands change if the barrier thickness is changed to 0.2 nm?
Finite Height Quantum Well: an Exercise for Band Structure
Use the Resonant Tunneling Diodes simulation tool on nanoHUB to explore the effects of finite height quantum wells.Looking at a 2 barrier device, 300 K, no bias, other standard variables, and 3 nm thick barriers and a 7 nm quantum well, determine the energies of the two lowest quasi-bound states.
MOSfet Homework Assignment - Role of Dielectric Constant and Thickness
Use the MOSfet tool on nanoHUB to simulate a n-channel MOSFET with the following parameters:Lsd=LG=45nm (each 15 nodes), oxide thickness of 1.2 nm (K=3.9, 5 nodes),poly-Si gate, junction depth of 10 nm (20 nodes), and all other parametersat their nominal preset values.Now, change K to 20, and...