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@PHDTHESIS{Vovchenko:211847,
author = {Vovchenko, Volodymyr},
othercontributors = {Stöcker, Horst},
title = {{Q}uantum statistical van der {W}aals equation and its
{QCD} applications},
school = {Johann Wolfgang Goethe-Universität Frankfurt},
type = {Dissertation},
reportid = {GSI-2018-00727},
pages = {xx, 146 S.},
year = {2018},
note = {Dissertation, Johann Wolfgang Goethe-Universität
Frankfurt, 2018},
abstract = {The theory of strong interactions — Quantum
Chromodynamics (QCD) — is well-defined mathematically.
However, direct applications of this theory to experiment
are rather limited due to significant technical obstacles.
Even some general features of QCD remain unclear to date.
Hence, phenomenological input is important and needed for
practical applications, e.g. for theoretical analysis of the
heavy-ion collision experiments. In this thesis the role of
hadronic interactions is studied in the hadron resonance gas
(HRG) model — a popular model for the confined phase of
QCD. The description of hadronic interactions is based on
the famous van der Waals (VDW) equation and its quantum
statistical generalization. While this is not the
conventional choice for nuclear/hadronic physicspplications,
the simplicity of the VDW approach makes it extremely
useful. In particular, this framework allows to include the
two most basic ingredients of hadron-hadron interaction: the
short-range repulsion, modeled by excluded-volume (EV)
corrections, and the intermediate range attraction. The
first part of the thesis considers just the repulsive EV
interactions between hadrons. A hitherto unknown, but
surprisingly strong sensitivity of the long known thermal
fits to heavy-ion hadron yield data to the choice of hadron
eigenvolumes is uncovered. It challenges the robustness of
the chemical freeze-out temperature and baryochemical
potential determination from the thermal fits. However, at
the same time, the extracted value of the entropy per baryon
is found to be a robust observable which depends weakly on
this systematic uncertainty of the HRG model.A Monte Carlo
procedure to treat EV interactions in HRG is also introduced
in this thesis. It allows to study simultaneous effects of
EV and of exact charge conservation in HRG for the first
time. Generalizations of the classical VDW equation are
required for its applications in hadronic physics. he grand
canonical ensemble (GCE) formulation of the classical VDW
equation is presented. Remarkably, this important aspect of
the VDW equation was not discovered before. The GCE
formulation yields the analytic structure of the critical
fluctuations, both in the vicinity of and far off the
critical point. These critical fluctuations are presently
actively being used as probes for the QCD critical point.
Another extension is the hitherto undiscovered
generalization of the VDW equation to include quantum
Bose-Einstein and Fermi-Dirac statistics. It is performed
for both single-component and multi-component fluids. The
Fermi-Dirac VDW equation is applied for the first time. It
is used to describe nucleons and basic properties of nuclear
matter. The quantum statistical generalization of the VDW
equation developed in this work is quite general, and can be
applied for any fluid. Thus, its applications are not
restricted to QCD physics, but may also find themselves in
chemistry and/or industry. The quantum statistical VDW
equation is used to describe baryonic interactions in full
HRG. The VDW parameters $a$ and $b$ are fixed to the nuclear
ground state and the predictions of the model are confronted
with lattice QCD calculations. The inclusion of baryonic
interactions leads to a qualitatively different behavior of
the fluctuations of conserved charges in the crossover
region. In many cases it resembles the lattice data. These
results suggest that hadrons do not melt quickly with
increasing temperature, as one could conclude on the basis
of the common simple ideal HRG model. Calculations at finite
chemical potentials show that the nuclear liquid-gas
transition manifests itself by non-trivial fluctuations of
the net baryon number in heavy ion collisions. In the final
part of the thesis the pure glue initial scenario for
high-energy hadron and heavy-ion collisions is explored.
This scenario is shown not to spoil the existing agreement
of the hadronic and electromagnetic observables description
in Pb+Pb collisions at energies available at the CERN Large
Hadron Collider. Hydrodynamic calculations suggest that
collisions of small-sized nuclei at lower collision energies
available at the BNL Relativistic Heavy Ion Collider are
promising in the search for the traces of the chemically
non-equilibrium gluon-dominated phase transition.},
cin = {THE},
cid = {I:(DE-Ds200)THE-20051214OR028},
pnm = {612 - Cosmic Matter in the Laboratory (POF3-612)},
pid = {G:(DE-HGF)POF3-612},
typ = {PUB:(DE-HGF)11},
urn = {urn:nbn:de:hebis:30:3-463016},
url = {https://repository.gsi.de/record/211847},
}