Lab Home | Phone | Search
Center for Nonlinear Studies  Center for Nonlinear Studies
 Home 
 People 
 Current 
 Executive Committee 
 Postdocs 
 Visitors 
 Students 
 Research 
 Publications 
 Conferences 
 Workshops 
 Sponsorship 
 Talks 
 Seminars 
 Postdoc Seminars Archive 
 Quantum Lunch 
 Quantum Lunch Archive 
 P/T Colloquia 
 Archive 
 Ulam Scholar 
 
 Postdoc Nominations 
 Student Requests 
 Student Program 
 Visitor Requests 
 Description 
 Past Visitors 
 Services 
 General 
 
 History of CNLS 
 
 Maps, Directions 
 CNLS Office 
 T-Division 
 LANL 
 
Thursday, January 28, 2010
12:30 PM - 2:00 PM
T-DO Conference Room, Bldg 123, Room 121

Quantum Lunch

Electronic Structure Calculations Using a New Density-Functional Theory

Gregory C. Dente
GCD Associates, Albuquerque, NM

In order to obtain a reasonably accurate and easily implemented approach to many-electron calculations, we will develop a new Density Functional Theory (DFT). Specifically, we derive an approximation to electron density, the first term of which is the Thomas-Fermi density, while the remaining terms substantially correct the density near the nucleus. As a first application, this new result allows us to accurately calculate the details of the self-consistent ion cores, as well as the ionization potentials for the outer s-orbital bound to the closed-shell ion core of the Group III, IV and V elements. Next, we demonstrate that the new DFT allows us to separate closed-shell core electron densities from valence electron densities. When we calculate the valence kinetic energy density, we show that it separates into two terms: the first exactly cancels the potential energy due to the ion core in the core region; the second represents the residual kinetic energy density resulting from the envelopes of the valence electron orbitals. This kinetic energy cancellation in the core region and the residual valence kinetic energy term allow us to write a functional for the total valence energy dependant only on the valence density. This equation provides the starting point for a large number of electronic structure calculations. Here, we use it to calculate the band structures of several Group IV and Group III-V semiconductors.

Host: Peter Miloni