Crystalline Solutions of Kohn-Sham Equations in the Fractional Quantum Hall Regime
arXiv:2102.12603 · doi:10.1103/PhysRevB.104.035122
Abstract
A Kohn-Sham density functional approach has recently been developed for the fractional quantum Hall effect, which maps the strongly interacting electrons into a system of weakly interacting composite fermions subject to an exchange correlation potential as well as a density dependent gauge field that mimics the "flux quanta" bound to composite fermions. To get a feel for the role of various terms, we study the behavior of the self-consistent solution as a function of the strength of the exchange correlation potential, which is varied through an {\it ad hoc} multiplicative factor. We find that a crystal phase is stabilized when the exchange correlation interaction is sufficiently strong relative to the composite-fermion cyclotron energy. Various properties of this crystal are examined.
10 pages, 5 figures; comments are welcome
References in corpus (8)
- A Density Matrix-based Algorithm for Solving Eigenvalue Problems
- Strong correlation in Kohn-Sham density functional theory
- Thirty Years of Composite Fermions and Beyond
- Wavefunctionology: The Special Structure of Certain Fractional Quantum Hall Wavefunctions
- Interpretations of ground-state symmetry breaking and strong correlation in wavefunction and density functional theories
- Composite fermion theory of correlated electrons in semiconductor quantum dots in high magnetic fields
- Kohn-Sham Density Functional Theory of Abelian Anyons
- Density Functional Theory of Composite Fermions
Cited by in corpus (4)
- Taming Landau level mixing in fractional quantum Hall states with deep learning
- Topological Protection in a Landau Flat Band at , a Candidate Filling Factor for Unconventional Correlations
- Developments in the applications of density functional theory to fractional quantum Hall systems
- Fermi energy sensitive universal conductance fluctuations in anisotropic materials