32 research outputs found
Can shadowing mimic the QCD phase transition?
The directed flow of protons is studied in the quark-gluon string model as a
function of the impact parameter for S+S and Pb+Pb reactions at 160 AGeV/c. A
significant reduction of the directed flow in midrapidity range, which can lead
to the development of the antiflow, is found due to the absorption of early
emitted particles by massive spectators (shadowing effect). This effect can
mimic the formation of the quark-gluon plasma (QGP). However, in the absorption
scenario the antiflow is stronger for the system of light colliding nuclei than
for the heavy ones, while in the case of the plasma creation the effect should
be opposite.Comment: REVTEX, 11 pages, 5 figures embedded, accepted for publication in
Physics Letters
Elliptic flow at RHIC: where and when does it formed?
Evolution of the elliptic flow of hadrons in heavy-ion collisions at RHIC
energies is studied within the microscopic quark-gluon string model. The
elliptic flow is shown to have a multi-component structure caused by (i)
rescattering and (ii) absorption processes in spatially asymmetric medium.
Together with different freeze-out dynamics of mesons and baryons, these
processes lead to the following trend in the flow formation: the later the
mesons are frozen, the weaker their elliptic flow, whereas baryon fraction
develops stronger elliptic flow during the late stages of the fireball
evolution. Comparison with the PHOBOS data demonstrates the model ability to
reproduce the v2(eta) signal in different centrality bins.Comment: 11 pages incl. 5 figure
Transition to meson-dominated matter at RHIC. Consequences for kaon flow
Anisotropic flow of kaons and antikaons is studied in heavy-ion collisions at
CERN SPS and BNL RHIC energies within the microscopic quark-gluon string model.
In the midrapidity range the directed flow of kaons v_1 differs considerably
from that of antikaons at SPS energy (E_{lab} = 160 AGeV), while at RHIC energy
(\sqrt{s} = 130 AGeV) the excitation functions of both, kaon and antikaon,
flows coincide within the statistical error bars. The change is attributed to
formation of dense meson-dominated matter at RHIC, where the differences in
interaction cross-sections of kaons and antikaons become unimportant. The time
evolution of the kaon anisotropic flow is also investigated. The elliptic flow
of these hadrons is found to develop at midrapidity at times 3 < t < 10 fm/c,
which is much larger than the nuclear passing time t^{pass} = 0.12 fm/c. As a
function of transverse momentum the elliptic flow increases almost linearly
with rising p_t. It stops to rise at p_t > 1.5 GeV/c reaching the saturation
value .Comment: REVTEX, 14 pages, 4 figure
Elliptic flow at collider energies and cascade string models: The role of hard processes and multi-Pomeron exchanges
Centrality, rapidity, and transverse momentum dependence of hadron elliptic
flow is studied in Au+Au collisions at BNL RHIC energies within the microscopic
quark-gluon string model. The QGSM predictions coincide well with the
experimental data at AGeV. Further investigations reveal that
multi-Pomeron exchanges and hard gluon-gluon scattering in primary collisions,
accompanied by the rescattering of hadrons in spatially anisotropic system, are
the key processes needed for an adequate description of the data. These
processes become essentially important for heavy-ion collisions at full RHIC
energy AGeV.Comment: LATEX, 12 pages incl. 4 figures, to be published in Phys. Lett.
Nucleation versus Spinodal decomposition in a first order quark hadron phase transition
We investigate the scenario of homogeneous nucleation for a first order
quark-hadron phase transition in a rapidly expanding background of quark gluon
plasma. Using an improved preexponential factor for homogeneous nucleation
rate, we solve a set of coupled equations to study the hadronization and the
hydrodynamical evolution of the matter. It is found that significant
supercooling is possible before hadronization begins. This study also suggests
that spinodal decomposition competes with nucleation and may provide an
alternative mechanism for phase conversion particularly if the transition is
strong enough and the medium is nonviscous. For weak enough transition, the
phase conversion may still proceed via homogeneous nucleation.Comment: LaTeX, 10 pages with 7 Postscript figures, more discussions and
referencese added, typos correcte
Homogeneous nucleation of quark-gluon plasma, finite size effects and long-lived metastable objects
The general formalism of homogeneous nucleation theory is applied to study
the hadronization pattern of the ultra-relativistic quark-gluon plasma (QGP)
undergoing a first order phase transition. A coalescence model is proposed to
describe the evolution dynamics of hadronic clusters produced in the nucleation
process. The size distribution of the nucleated clusters is important for the
description of the plasma conversion. The model is most sensitive to the
initial conditions of the QGP thermalization, time evolution of the energy
density, and the interfacial energy of the plasma-hadronic matter interface.
The rapidly expanding QGP is first supercooled by about . Then it reheats again up to the critical temperature T_c. Finally it
breaks up into hadronic clusters and small droplets of plasma. This fast
dynamics occurs within the first . The finite size effects and
fluctuations near the critical temperature are studied. It is shown that a drop
of longitudinally expanding QGP of the transverse radius below 4.5 fm can
display a long-lived metastability. However, both in the rapid and in the
delayed hadronization scenario, the bulk pion yield is emitted by sources as
large as 3-4.5 fm. This may be detected experimentally both by a HBT
interferometry signal and by the analysis of the rapidity distributions of
particles in narrow p_T-intervals at small p_T on an event-by-event basis.Comment: 29 pages, incl. 12 figures and 1 table; to be published in Phys. Rev.
Vacuum creation of quarks at the time scale of QGP thermalization and strangeness enhancement in heavy-ion collisions
The vacuum parton creation in quickly varying external fields is studied at
the time scale of order 1 fm/ typical for the quark-gluon plasma formation
and thermalization. To describe the pre-equilibrium evolution of the system the
transport kinetic equation is employed. It is shown that the dynamics of
production process at times comparable with particle inverse masses can deviate
considerably from that based on classical Schwinger-like estimates for
homogeneous and constant fields. One of the effects caused by non-stationary
chromoelectric fields is the enhancement of the yield of quark
pairs. Dependence of this effect on the shape and duration of the field pulse
is studied together with the influence of string fusion and reduction of quark
masses.Comment: REVTEX, 11pp. incl. 4 figures, to be published in Phys. Lett.
Non-perturbative effects in a rapidly expanding quark-gluon plasma
Within first-order phase transitions, we investigate the pre-transitional
effects due to the nonperturbative, large-amplitude thermal fluctuations which
can promote phase mixing before the critical temperature is reached from above.
In contrast with the cosmological quark-hadron transition, we find that the
rapid cooling typical of the RHIC and LHC experiments and the fact that the
quark-gluon plasma is chemically unsaturated suppress the role of
non-perturbative effects at current collider energies. Significant supercooling
is possible in a (nearly) homogeneous state of quark gluon plasma.Comment: LaTeX, 7 pages with 7 Postscript figures. Figures added, discussions
added. Version to appear in Phys. Rev.
Partonic effects on the elliptic flow at relativistic heavy ion collisions
The elliptic flow in heavy ion collisions at RHIC is studied in a multiphase
transport model. By converting the strings in the high energy density regions
into partons, we find that the final elliptic flow is sensitive to the parton
scattering cross section. To reproduce the large elliptic flow observed in
Au+Au collisions at GeV requires a parton scattering cross
section of about 6 mb. We also study the dependence of the elliptic flow on the
particle multiplicity, transverse momentum, and particle mass.Comment: 7 pages, 7 figures, revtex, text added to detail the procedure for
conversions between hadrons and parton
Chemical freeze-out of light nuclei in high energy nuclear collisions and resolution of the hyper-Triton chemical freeze-out puzzle
Indexación ScopusWe present a summary of the recent results obtained with the novel hadron resonance gas model with the multicomponent hard-core repulsion which is extended to describe the mixtures of hadrons and light (anti-, hyper-)nuclei. A very accurate description is obtained for the hadronic and the light nuclei data measured by STAR at the collision energy The most striking result discussed here is that for the most probable chemical freeze-out scenario for the STAR energy the found parameters allow us to reproduce the values of the experimental ratios S 3 and without fitting. © Published under licence by IOP Publishing Ltd.https://iopscience-iop-org.recursosbiblioteca.unab.cl/article/10.1088/1742-6596/1690/1/01212