Quasiparticle self-consistent method; a basis for the independent-particle approximation
arXiv:cond-mat/0611002 · doi:10.1103/PhysRevB.76.165106
Abstract
We have developed a new type of self-consistent scheme within the approximation, which we call quasiparticle self-consistent (QS). We have shown that QS rather well describes energy bands for a wide-range of materials, including many where the local-density approximation fails. QS contains physical effects found in other theories such as LDA, SIC and in a satisfactory manner without many of their drawbacks (partitioning of itinerant and localized electrons, adjustable parameters, ambiguities in double-counting, etc.). We present some theoretical discussion concerning the formulation of QS, including a prescriptino for calculating the total energy. We also address several key methodological points needed for implementation. We then show convergence checks and some representative results in a variety of materials.
v2:the same as previous version --but better tex file; v3:add appendix and modify introduction,mainly; v4 mainly, theoretical section (IB IC) are renewed
Cited by in corpus (8)
- GW method applied to localized 4f electron systems
- Spin wave dispersion based on the quasiparticle self-consistent method: NiO, MnO and -MnAs
- Many-body Electronic Structure of Metallic alpha-Uranium
- Effective Coulomb interactions in solids under pressure
- Strain-Induced Conduction Band Spin Splitting in GaAs from First Principles Calculations
- Combining the Hybrid Functional Method with Dynamical Mean-Field Theory
- Re-examination of half-metallic ferromagnetism for doped LaMnO3 in quasiparticle self-consistent method
- GW correlation effects on plutonium quasiparticle energies: changes in crystal-field splitting