1,107 research outputs found
Eccentricity fluctuations in an integrated hybrid approach: Influence on elliptic flow
The effects of initial state fluctuations on elliptic flow are investigated
within a (3+1)d Boltzmann + hydrodynamics transport approach. The spatial
eccentricity ( and ) is calculated for
initial conditions generated by a hadronic transport approach (UrQMD). Elliptic
flow results as a function of impact parameter, beam energy and transverse
momentum for two different equations of state and for averaged initial
conditions or a full event-by-event setup are presented. These investigations
allow the conclusion that in mid-central ( fm) heavy ion collisions the
final elliptic flow is independent of the initial state fluctuations and the
equation of state. Furthermore, it is demonstrated that most of the is
build up during the hydrodynamic stage of the evolution. Therefore, the use of
averaged initial profiles does not contribute to the uncertainties of the
extraction of transport properties of hot and dense QCD matter based on viscous
hydrodynamic calculations.Comment: 7 pages, 7 figures, minor revision of figures and conclusion, as
published in PR
Hadronization conditions in relativistic nuclear collisions and the QCD pseudo-critical line
We compare the reconstructed hadronization conditions in relativistic nuclear
collisions in the nucleon-nucleon centre-of-mass energy range 4.7-2760 GeV in
terms of temperature and baryon-chemical potential with lattice QCD
calculations, by using hadronic multiplicities. We obtain hadronization
temperatures and baryon chemical potentials with a fit to measured
multiplicities by correcting for the effect of post-hadronization rescattering.
The post-hadronization modification factors are calculated by means of a
coupled hydrodynamical-transport model simulation under the same conditions of
approximate isothermal and isochemical decoupling as assumed in the statistical
hadronization model fits to the data. The fit quality is considerably better
than without rescattering corrections, as already found in previous work. The
curvature of the obtained "true" hadronization pseudo-critical line kappa is
found to be 0.0048 +- 0.0026, in agreement with lattice QCD estimates; the
pseudo-critical temperature at vanishing mu_B is found to be 164.3+-1.8 MeV.Comment: 9 pages, 2 figures. Minor corrections, version published in PL
Resonance Production in RHIC Collisions
Results of resonance particle production measured at RHIC in 200 GeV Au+Au collisions are compared to measurements in p+p and d+Au
collisions in order to verify the existence of an extended hardronically
interacting medium. Yield and momentum distributions of resonances maybe
modified during the fireball lifetime due to resonance decay and the subsequent
rescattering of their decay daughters as well as the regeneration of resonances
from their decay products. Modified momentum spectra in heavy ion collisions
may change the nuclear modification factor R. The influence on the
elliptic flow v due to late regeneration of resonances is discussed.Comment: 6 pages, 6 figures, Proceedings of the 22st Winter Workshop on
Nuclear Dynamics, San Diago, California, 12-18 March, 200
A model comparison of resonance lifetime modifications, a soft equation of state and non-Gaussian effects on correlations at FAIR/AGS energies
HBT correlations of pairs at FAIR/AGS energies are investigated
by using the UrQMD transport model and the CRAB analyzing program. Three
different possible sources (treatment of resonance lifetimes, a soft equation
of state and non-Gaussian effects) to understand the HBT puzzle are
investigated. Firstly, we find that different treatments of the resonance decay
time can not resolve the HBT time-related puzzle, however it can modify the HBT
radii at low transverse momenta to some extent to explain the data slightly.
Secondly, with a soft equation of state with momentum dependence, the measured
transverse momentum dependent HBT radii and ratio can be described
fairly well. Thirdly, non-Gaussian effects are visible in the calculated
correlation function. Using the Edgeworth expansion, one finds that the
non-Gaussian effect is strongest in the longitudinal direction and weakest in
the sideward direction.Comment: 18 pages, 6 figures. To be published in J.Phys.
Lattice QCD and Hydro/Cascade Model of Heavy Ion Collisions
We report here on a recent lattice study of the QCD transition region at
finite temperature and zero chemical potential using domain wall fermions
(DWF). We also present a parameterization of the QCD equation of state obtained
from lattice QCD that is suitable for use in hydrodynamics studies of heavy ion
collisions. Finally, we show preliminary results from a multi-stage
hydrodynamics/hadron cascade model of a heavy ion collision, in an attempt to
understand how well the experimental data (e.g. particle spectra, elliptic
flow, and HBT radii) can constrain the inputs (e.g. initial temperature,
freezeout temperature, shear viscosity, equation of state) of the theoretical
model.Comment: 10 pages, 12 figures. Proceedings for the 26th Winter Workshop on
Nuclear Dynamics, Ocho Rios, Jamaica, Jan 2-9, 201
Hadronic Freeze-Out in A+A Collisions meets the Lattice QCD Parton-Hadron Transition Line
We analyze hadrochemical freeze-out in central Pb+Pb collisions at CERN SPS
and LHC energies. Employing the UrQMD hybrid transport model we study the
effects of the final hadron/resonance expansion phase on the hadron
multiplicities established at hadronization. The bulk meson yields freeze out
directly at hadronization whereas the baryon-antibaryon sector is subject to
significant alterations, due to annihilation and regeneration processes. We
quantify the latter changes by survival factors for each species which are
applied to modify the statistical model predictions for the data. The modified
SM analysis recovers the hadronization points, which coincide with the recent
lattice QCD predictions of the parton-hadron transition line at finite
baryochemical potential.Comment: Proceedings of the 8th International Workshop on Critical Point and
Onset of Deconfinement, March 11 to 15, 2013 Napa, California, US
Dynamics and freeze-out of hadron resonances at RHIC
Yields, rapidity and transverse momentum spectra of ,
, and the meson resonances ,
, and are predicted. Hadronic rescattering leads to a
suppression of reconstructable resonances, especially at low . A mass
shift of the of 10 MeV is obtained from the microscopic simulation, due
to late stage formation in the cooling pion gas.Comment: Proceedings of the Strange Quark Matter 2003, eprint version differs
from published versio
Evapotranspiração e coeficientes de cultivo e de irrigação para a cultura do melão (Cucumis melo L.) na região litorânea do Ceará.
O experimento foi conduzido em Paraipaba, Regiao Litoranea do Ceara (latitude 3°17 S, longitude 3°15 W e altitude de 30m), com objetivo de determinar a evapotranspiracao (ETc) e os coeficientes de cultivo (Kc) e de irrigacao (Ki) para as diferentes fases da cultura do melao (Cucumis melo L.).Utilizou-se o melao hibrido amarelo Gold Mine, no espacamento de 2,0 x 0,5m, irrigado diariamente, por gotejamento, com uma linha de gotejadores por fileiras de plantas, espaçados de 0,5m entre si. Para determinar a ETc da cultura do melao utilizou-se um lizimetro de pesagem com area superficial de 2,25 m² (1,5 x 1,5m) , instalada no centro de uma area cultivada de 110 x 70m.Os valores de ETc diaria obtidos foram comparados com valores de ETc determinados diretamente por outro lisimetro de pesagem e estimado pelo metodo de Penman-Monteith e valores de evaporacao diaria do tanque classe "A". O ciclo total da cultura foi de 66 dias e as duracoes de fases inicial, de crescimento, intermediaria e final da cultura foram de 23,18,18 e 7 dias, respectivamente. A ETc total durante o ciclo do meloeiro foi de 251 mm e o periodo de maxima demanda hidrica ocorreo entre 42 e 58 dias apos o plantio, com valores maximos de ETc de ate 6,8 mm/dia . Foram verificados valores medios de Kc de 0,21 na fase inicial, 1,21 na fase intermediaria e 0,98 na fase final, calculados com valores de ETo determinados por lisimetro de pesagem, que praticamente nao diferiram dos Kc s calculados com valores de ETo estimado pelo metodo de Penman-Monteith. Os valores de Ki observados foramde 0,13 na fase inicial, 0,68 na fase intermediaria e 0,55 na fase final.bitstream/CNPAT-2010/9009/1/Bd-002.pd
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