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@PHDTHESIS{Rodekamp:1030406,
author = {Rodekamp, Marcel},
title = {{M}achine {L}earning for {P}ath {D}eformation and
{B}ayesian {D}ata {A}nalysis in {S}elected {L}attice {F}ield
{T}heories},
school = {Bonn},
type = {Dissertation},
address = {Bonn},
publisher = {Universitäts- und Landesbibliothek Bonn: bonndoc},
reportid = {FZJ-2024-05279},
pages = {151},
year = {2024},
note = {Dissertation, Bonn, 2024},
abstract = {Our collective understanding of the laws of nature has a
long history of an intricate interplay between theoretical
considerations and experimental falsification. As
computational power increases, simulations, at the interface
between theory and experiment, have taken an increasing role
in scientific discovery. In particular, first-principles
calculations are indispensable for systems with
non-perturbative behavior, requiring simulations to test
models against experiment. One widely accepted and deployed
method involves formulating the theory on a finite lattice
and then applying a Monte Carlo simulation. However, with
increasing interest in such simulations practical and
fundamental challenges arise, such as computational demand
and the numerical sign problem. In the following, I discuss
selected aspects for simulations of strongly correlated
systems, namely the Hubbard model and lattice quantum
chromodynamics. This encompasses methods to mitigate the
numerical sign problem and (Bayesian) analysis of simulation
results, in particular fitting methods and the treatment of
excited state contamination.The Hubbard model describes
systems of strongly correlated electrons and is used often
in studying chemical compounds. First principle studies of
this model are almost exclusively done using Monte Carlo
techniques, with the exception being very small systems
where direct diagonalization methods are feasible. However,
away from half filling, Monte Carlo methods struggle because
of the numerical sign problem. While the sign problem is
unlikely to be completely solved, methods that reduce its
impact are very valuable in expanding the computable
parameter space. Leveraging theoretical developments on path
deformations, I demonstrate that machine learning techniques
can be used to mitigate the sign problem. In particular, I
train complex-valued neural networks to serve as a
parameterization of a sign-optimized manifold related to
Lefschetz thimbles. These methods were developed and tested
on doped graphene sheets, modelled by a small number of ions
with periodic boundary conditions, at fixed temporal
discretization and temperature.Renewable energy is a
critical aspect of modern research to reduce effects of
climate change. Despite the enormous energy cost of
producing solar panels, they are a valuable element in the
electricity production. Organic solar cells show great
promise in reducing costs and allowing for flexibility.
Unfortunately, to date their efficiency falls behind their
silicon-based competitors. By studying the electronic
structure of certain chemical compounds that are usable for
organic solar cells, further development in this area can be
fostered. This motivates my work in the molecule C20 H12
perylene, which can be used as an acceptor material in
organic solar cells. This molecule is typically not at half
filling, so any simulation requires methods to mitigate the
sign problem.The study of perylene shown here requires the
analysis of a large data set, of the order of O (2000)
correlators, which is only feasible with an automated
analysis procedure. In this thesis I present such an
automatic routine based on Bayesian analysis using the
Akaike information criterion.Finally, I shift the focus to
particle physics to calculate aspects of the internal
structure of hadrons. Hadrons are primarily governed by the
strong interaction, i.e. described by quantum chromodynamics
(QCD). In this theory, the internal structure is modelled by
the correlation between spatial and momentum distributions
of all constituents. Many details of these distributions
remain to be calculated. In this thesis, I use lattice QCD
to calculate the 2nd moment of parton distribution functions
(PDFs) for the nucleon. These are the average momentum
fractions carried by the considered parton of the nucleon. I
analyze two ensembles at the physical pion mass to obtain
the moments of unpolarized, polarized, and transversity PDF
for the nucleon.},
cin = {JSC / CASA},
cid = {I:(DE-Juel1)JSC-20090406 / I:(DE-Juel1)CASA-20230315},
pnm = {5111 - Domain-Specific Simulation $\&$ Data Life Cycle Labs
(SDLs) and Research Groups (POF4-511) / SDS005 - Towards an
integrated data science of complex natural systems
(PF-JARA-SDS005)},
pid = {G:(DE-HGF)POF4-5111 / G:(DE-Juel-1)PF-JARA-SDS005},
typ = {PUB:(DE-HGF)11},
doi = {10.34734/FZJ-2024-05279},
url = {https://juser.fz-juelich.de/record/1030406},
}