Correlation energy extrapolation by intrinsic scaling. III. Compact wave functions

2004 ◽  
Vol 121 (22) ◽  
pp. 10852 ◽  
Author(s):  
Laimutis Bytautas ◽  
Klaus Ruedenberg
Keyword(s):  
Correlation Energy ◽  
Wave Functions ◽  
Energy Extrapolation

Improvement of Multiconfigurational Wave Functions and Energies by Correlation Energy Functionals

1998 ◽  
Vol 102 (52) ◽  
pp. 10900-10902 ◽  
Author(s):  
Federico Moscardó ◽  
Francisco Muñoz-Fraile ◽  
Angel J. Pérez-Jiménez ◽  
José M. Pérez-Jordá ◽  
Emilio San-Fabián
Keyword(s):  
Correlation Energy ◽  
Wave Functions ◽  
Energy Functionals

scholarly journals Correlation Energy Extrapolation by Many-Body Expansion

2017 ◽  
Vol 121 (4) ◽  
pp. 836-844 ◽  
Author(s):  
Jeffery S. Boschen ◽  
Daniel Theis ◽  
Klaus Ruedenberg ◽  
Theresa L. Windus
Keyword(s):  
Correlation Energy ◽  
Many Body ◽  
Energy Extrapolation

Size-consistent wave functions for nondynamical correlation energy: The valence active space optimized orbital coupled-cluster doubles model

1998 ◽  
Vol 109 (24) ◽  
pp. 10669-10678 ◽  
Author(s):  
Anna I. Krylov ◽  
C. David Sherrill ◽  
Edward F. C. Byrd ◽  
Martin Head-Gordon
Keyword(s):  
Correlation Energy ◽  
Wave Functions ◽  
Coupled Cluster ◽  
Active Space

Efficient Electronic Energy Functionals for Tight-Binding

1997 ◽  
Vol 491 ◽  
Author(s):  
Roger Haydock
Keyword(s):  
Ground State ◽  
State Energy ◽  
Correlation Energy ◽  
Tight Binding ◽  
Electronic Energy ◽  
Wave Functions ◽  
Electronic Charge ◽  
Energy Functionals ◽  
Exchange Correlation ◽  
Band Structure Energy

ABSTRACTGeneralized functionals are constructed from the exchange-correlation energy by a Legendre transformation which makes the new functionals stationary at the electronic charge density, potential, and wave functions for the ground-state. Using generalized functionals, the density, potential, and wave functions can be independently parameterized and varied to determine the ground-state energy-surface for a system of atoms. This eliminates the computationally awkward steps of constructing densities from wave functions or potentials from densities, and is particularly well suited to parameterizations using tight-binding orbitale together with atomic-like densities and potentials. For each choice of parameters, the only quantities which must be computed are the electron-electron energy for the density, the integral of the potential over the density, and the band structure energy for the wave functions. To second order in the density, potential, and wave functions, the energy for a configuration of atoms is given by the generalized functional evaluated at a superposition of atomic densities, a potential made by stitching together the atomic potentials where they are equal, and atomic wave functions. For more accurate stationary energies the densities, potentials, and wave functions can be improved by one or more conjugate gradient steps.

Sign in / Sign up

Export Citation Format

Share Document