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@PHDTHESIS{Zhang:878578,
author = {Zhang, Qian},
title = {{B}uilding {E}ffective {M}odels for {C}orrelated {E}lectron
{S}ystems},
school = {RWTH Aachen University},
type = {Dissertation},
reportid = {FZJ-2020-02921},
pages = {227 pages},
year = {2020},
note = {Dissertation, RWTH Aachen University, 2020},
abstract = {To understand strongly correlated systems, we must confront
the many-body problem. This is practically impossible for
the ab-initio Hamiltonian. To make such studies feasible it
is, thus, crucial to construct model Hamiltonians that are
as simple as possible, so they can be solved, while
containing still enough details to be material-specific.Our
starting point is density functional theory for individual
atoms and ions to obtain re- alistic basis functions and the
corresponding matrix elements. For the open-shell orbitals,
which show the strongest correlation effects due to the
degeneracy of the multiplets, we calculate the Slater-Condon
and spin-orbit parameters from the resulting self-consistent
radial wave functions and potentials. We study the trends of
the parameters systemati- cally across the periodic table,
develop an intuitive parametrization, and calculate atomic
open-shell spectra in LS-, intermediate-, and jj-coupling
schemes.The comparison of the interaction strengths of
different coupling schemes gives rise to the study of the
moment formulas, which reduce the calculation from the
“impossible” many-electron Hilbert space to a one- or
two-electron space. We derive the analytic moment formulas
for the general one- and two-body Hamiltonians. The moment
formulas provide us a new approach to handle the
many-electron Hamiltonians without the need of working with
a many-electron basis, but only with matrix representations
under the one- or two-electron basis.To model the
Hamiltonians for realistic materials, orthonormal basis
orbitals are preferred. However, while the atomic orbitals
are mutually orthonormal within a single atom, they are, in
general, non-orthogonal for atoms on different lattice
sites. We study and develop efficient multi-center integral
techniques for evaluating orbital overlaps, which are essen-
tial for performing the orbital orthogonalization. To
orthogonalize the basis orbitals, we apply the Löwdin
symmetric orthogonalization scheme, which minimizes the
orbital modification. To generalize the multi-center
integrals, we introduce the re-centering method, which is a
spherical harmonic expansion that requires the Gaunt
coefficients with large angular quantum numbers. To compute
the Gaunt coefficients, the previously known numerical
methods are, however, inaccurate for the coefficients that
involve large quantum numbers. Therefore, we provide a
numerically stable algorithm for computing the Gaunt
coefficients efficiently and accurately. The re-centering
method enables us to compute general multi-center integrals
including the hopping matrix elements and the long-range
Coulomb matrix elements. After performing the basis
orthonormalization, we study the deformation of the
resulting orbitals and investigate the modification of the
corresponding multi-center matrix elements under changes of
the bond lengths or lattice constants.},
cin = {JSC},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {511 - Computational Science and Mathematical Methods
(POF3-511)},
pid = {G:(DE-HGF)POF3-511},
typ = {PUB:(DE-HGF)11},
url = {https://juser.fz-juelich.de/record/878578},
}