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@PHDTHESIS{Hasan:874258,
author = {Hasan, Nesreen},
title = {{A} lattice {QCD} study of nucleon structure with physical
quark masses},
volume = {41},
school = {Universität Wuppertal},
type = {Dr.},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2020-01349},
isbn = {978-3-95806-456-0},
series = {Schriften des Forschungszentrums Jülich. Reihe IAS Series},
pages = {xiii, 157 S.},
year = {2020},
note = {Universität Wuppertal, 2019},
abstract = {In this work, we compute various nucleon structure
observables using the lattice regularization of quantum
chromodynamics, lattice QCD. Our calculations are performed
using 2 + 1-flavor ensembles with clover-improved Wilson
fermions and cover three sets of abserbales: The first set
includes the computation of nucleon isovector axial, scalar,
and tensor charges. In particular, we focus on controlling
the unwanted contributions from excited states. Those
charges quantify the coupling of nucleons to quark-level
interactions and play an important role in the analysis of
the Standard Model and Beyond the Standard Model (BSM)
physics. The second set of observables includes the nucleon
charge and axial radii measured using a new and
model-independent approach. We developed this approach to
enable the computation of the nucleon radii directly at zero
momentum transfer and avoid the systematic uncertainty
orginating from the large extrapolation commonly included in
the conventional methods used for measuring quantities like
the nucleon charge radius. Systematic errors of this kind
have been proposed as a possible explanation of the radius
puzzle which refers to the > 5$\sigma$ discrepancy between
the experimental electronic and muonic determinations of the
charge radius of the proton. We perform the calculations of
the nucleon charges and radii on two gauge ensembles at the
physical pion mass and with different lattice spacings. The
last set of our calculation is devoted to measuring the
nucleon axial form factors. This calculation includes both
quark-connected and -disconnected diagrams, which allows us
to determine the up, down, and strange form factors. This
calculation is done using a single ensemble with pion mass
317 MeV.},
cin = {JSC},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {511 - Computational Science and Mathematical Methods
(POF3-511) / PhD no Grant - Doktorand ohne besondere
Förderung (PHD-NO-GRANT-20170405)},
pid = {G:(DE-HGF)POF3-511 / G:(DE-Juel1)PHD-NO-GRANT-20170405},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
urn = {urn:nbn:de:0001-2020012307},
url = {https://juser.fz-juelich.de/record/874258},
}