
Resonant Tunneling Diode Simulation with NEGF: FirstTime User Guide
01 Jun 2009   Contributor(s):: Samarth Agarwal, Gerhard Klimeck
This firsttime user guide for Resonant Tunneling Diode Simulation with NEGF provides some fundamental concepts regarding RTDs along with details on how device geometry and simulation parameters influence current and charge distribution inside the device.NCN@Purdue

ECE 659 Lecture 42: Summing Up
04 May 2009   Contributor(s):: Supriyo Datta

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.

ECE 659 Lecture 36: Law of Equilibrium
01 May 2009   Contributor(s):: Supriyo Datta

ECE 659 Lecture 18: NEGF Equations
03 Mar 2009   Contributor(s):: Supriyo Datta

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 NonEquilibrium Green's Functions

OMEN Nanowire
02 Sep 2008   Contributor(s):: SungGeun Kim, Mathieu Luisier, Benjamin P Haley, Abhijeet Paul, Saumitra Raj Mehrotra, Gerhard Klimeck, Hesameddin Ilatikhameneh
Fullband 3D quantum transport simulation in nanowire structure

ECE 495N Lecture 34: NEGF Continued I
10 Dec 2008   Contributor(s):: Supriyo Datta

ECE 495N Lecture 35: NEGF Continued II
10 Dec 2008   Contributor(s):: Supriyo Datta

ECE 495N Lecture 33: NonEquilibrium Green's Function (NEGF) Method
04 Dec 2008   Contributor(s):: Supriyo Datta

NanoTCAD ViDES
24 Jul 2008   Contributor(s):: Gianluca Fiori, Giuseppe Iannaccone
3D Poisson/NEGF solver for the simulation of Graphene Nanoribbon, Carbon nanotubes and Silicon Nanowire Transistors.

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 selfconsistent fields and the hydrodynamic equations for acoustic and optical phonons. The phonon...

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
02 Sep 2008   Contributor(s):: Supriyo Datta
Objective: To incorporate distributed energy exchange processes into the previous models from lectures 1 through 3 which are based on a "Landauerlike picture" where the Joule heating associated with current flow occurs entirely in the two contacts.Although there is experimental evidence that...

Introduction: Nanoelectronics and the meaning of resistance
20 Aug 2008   Contributor(s):: Supriyo Datta
This lecture provides a brief overview of the fiveday short course whose purpose is to introduce a unified viewpoint for a wide variety of nanoscale electronic devices of great interest for all kinds of applications including switching, energy conversion and sensing. Our objective, however, is...

Lecture 2A: Quantum Transport
20 Aug 2008   Contributor(s):: Supriyo Datta
Objective: To extend the simple model from Lectures 1 into the fullfledged Nonequilibrium Green’s Function (NEGF) – Landauer model by introducing a spatial grid of N points and turning numbers like into (NxN) matrices like , with incoherent scattering introduced through . This model will be...

Lecture 2B: Quantum Transport
20 Aug 2008   Contributor(s):: Supriyo Datta
Objective: To extend the simple model from Lectures 1 into the fullfledged Nonequilibrium Green’s Function (NEGF) – Landauer model by introducing a spatial grid of N points and turning numbers like into (NxN) matrices like , with incoherent scattering introduced through . This model will be...

Lecture 3A: Spin Transport
20 Aug 2008   Contributor(s):: Supriyo Datta
Objective: To extend the model from Lectures 1 and 2 to include electron spin. Every electron is an elementary “magnet” with two states having opposite magnetic moments. Usually this has no major effect on device operation except to increase the conductance by a factor of two.But it is now...

Lecture 3B: Spin Transport
20 Aug 2008   Contributor(s):: Supriyo Datta
Objective: To extend the model from Lectures 1 and 2 to include electron spin. Every electron is an elementary “magnet” with two states having opposite magnetic moments. Usually this has no major effect on device operation except to increase the conductance by a factor of two.But it is now...

Lecture 4B: Energy Exchange and Maxwell’s Demon
20 Aug 2008   Contributor(s):: Supriyo Datta
Objective: To incorporate distributed energy exchange processes into the previous models from lectures 1 through 3 which are based on a “Landauerlike picture” where the Joule heating associated with current flow occurs entirely in the two contacts.Although there is experimental evidence that...