Abstract

Self-consistent calculations using the Perdew-Zunger self-interaction correction (PZ-SIC) to local density and gradient dependent energy functionals are presented for the binding energy and equilibrium geometry of small molecules as well as energy barriers of reactions. The effect of the correction is to reduce binding energy and bond lengths and increase activation energy barriers when bond breaking is involved. The accuracy of the corrected functionals varies strongly, the correction to the binding energy being too weak for the local density approximation but too strong for the gradient dependent functionals considered. For the Perdew, Burke, and Ernzerhof (PBE) functional, a scaling of the PZ-SIC by one half gives improved results on average for both binding energy and bond lengths. The PZ-SIC does not necessarily give more accurate total energy, but it can result in a better cancellation of errors. An essential aspect of these calculations is the use of complex orbitals. A restriction to real orbitals leads to less accurate results as was recently shown for atoms [S. Klüpfel, P. Klüpfel, and H. Jónsson, Phys. Rev. A 84, 050501 (2011)]. The molecular geometry of radicals can be strongly affected by PZ-SIC. An incorrect, non-linear structure of the C(2)H radical predicted by PBE is corrected by PZ-SIC. The CH(3) radical is correctly predicted to be planar when complex orbitals are used, while it is non-planar when the PZ-SIC calculation is restricted to real orbitals.

Highlights

  • Implementation of a self-consistent treatment of SIC functionals in Quantice made it possible to carry out a reliable minimization of the energy, using the unitary optimization algorithm developed in our group

  • The total energy is most affected by extending the variational space from real to complex orbitals, as illustrated by the atomic calculations

  • In contrast to previous results based on real orbitals, Perdew-Zunger self-interaction correction (PZ-SIC) can improve the total energy when it is applied to generalized gradient approximation (GGA) functionals

Read more

Summary

Theoretical Background

The accurate description of systems on a molecular or atomic level cannot be achieved by means of classical mechanics, as quantum effects have to be accounted for. Theoretical Background systems depends on the coordinates of N electrons, {r}, and of M nuclei, {R} For such a system the potential operator Vis built up from different contributions: Nucleus-nucleus repulsion (Vnn), nucleus-electron attraction (Vne), electron-electron repulsion (Vee) and, possibly, the interaction of the particles with an external electrostatic field (V0). The nuclear kinetic energy operator has an action on the electronic wavefunction, as it depends on the nuclear coordinates in a parametric way. The computation of the wavefunction and energy of a system made up of nuclei and electrons can be separated into an electronic and a nuclear problem These two are connected via the potential energy surface, whose computation is in most cases a challenging task. This is infeasible, both analytically and even numerically, for most electronic systems

Hohenberg-Kohn Density Functional Theory
Kohn-Sham Density Functional Theory
Density Functional Approximations
B88 Exchange Functional
Shortcomings of Approximate Functionals
Perdew-Zunger
Definition
Perdew-Zunger Self-Interaction Correction
Self-Consistent Minimization
Previous Assessment
Scaled Self-Interaction Correction
Implementation of Perdew-Zunger Self-Interaction Correction
Complex Orbitals
Unitary Optimization Algorithm
Quantice
Numerical results
Atomic Systems
Molecular Systems
H4 HFH
Summary and Outlook
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call