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Baryon Number, Strangeness and Electric Charge Fluctuations in QCD at High Temperature
Cheng, M.;Hegde, P.;Jung, C.;Karsch, F.;Kaczmarek, O.;Laermann, E.;Mawhinney, R. D.;Miao, C.;Petreczky, P.;Schmidt, C.;Soeldner, W.
High Energy Physics - Phenomenology , 2008,
Abstract: We analyze baryon number, strangeness and electric charge fluctuations as well as their correlations in QCD at high temperature. We present results obtained from lattice calculations performed with an improved staggered fermion action (p4-action) at two values of the lattice cut-off with almost physical up and down quark masses and a physical value for the strange quark mass. We compare these results, with an ideal quark gas at high temperature and a hadron resonance gas model at low temperature. We find that fluctuations and correlations are well described by the former already for temperatures about 1.5 times the transition temperature. At low temperature qualitative features of the lattice results are quite well described by a hadron resonance gas model. Higher order cumulants, which become increasingly sensitive to the light pions, however show deviations from a resonance gas in the vicinity of the transition temperature.
Baryon Number, Strangeness and Electric Charge Fluctuations in QCD at High Temperature  [PDF]
M. Cheng,P. Hegde,C. Jung,F. Karsch,O. Kaczmarek,E. Laermann,R. D. Mawhinney,C. Miao,P. Petreczky,C. Schmidt,W. Soeldner
Physics , 2008, DOI: 10.1103/PhysRevD.79.074505
Abstract: We analyze baryon number, strangeness and electric charge fluctuations as well as their correlations in QCD at high temperature. We present results obtained from lattice calculations performed with an improved staggered fermion action (p4-action) at two values of the lattice cut-off with almost physical up and down quark masses and a physical value for the strange quark mass. We compare these results, with an ideal quark gas at high temperature and a hadron resonance gas model at low temperature. We find that fluctuations and correlations are well described by the former already for temperatures about 1.5 times the transition temperature. At low temperature qualitative features of the lattice results are quite well described by a hadron resonance gas model. Higher order cumulants, which become increasingly sensitive to the light pions, however show deviations from a resonance gas in the vicinity of the transition temperature.
Fluctuations and Correlations of net baryon number, electric charge, and strangeness: A comparison of lattice QCD results with the hadron resonance gas model  [PDF]
A. Bazavov,Tanmoy Bhattacharya,C. E. DeTar,H. -T. Ding,Steven Gottlieb,Rajan Gupta,P. Hegde,Urs Heller,F. Karsch,E. Laermann,L. Levkova,Swagato Mukherjee,P. Petreczky,Christian Schmidt,R. A. Soltz,W. Soeldner,R. Sugar,Pavlos M. Vranas
Physics , 2012, DOI: 10.1103/PhysRevD.86.034509
Abstract: We calculate the quadratic fluctuations of net baryon number, electric charge and strangeness as well as correlations among these conserved charges in (2+1)-flavor lattice QCD at zero chemical potential. Results are obtained using calculations with tree level improved gauge and the highly improved staggered quark (HISQ) actions with almost physical light and strange quark masses at three different values of the lattice cut-off. Our choice of parameters corresponds to a value of 160 MeV for the lightest pseudo scalar Goldstone mass and a physical value of the kaon mass. The three diagonal charge susceptibilities and the correlations among conserved charges have been extrapolated to the continuum limit in the temperature interval 150 MeV
Bulk thermodynamics and charge fluctuations at non-vanishing baryon density  [PDF]
Chuan Miao,Christian Schmidt
Physics , 2007,
Abstract: We present results on bulk thermodynamic quantities as well as net baryon number, strangeness and electric charge fluctuations in QCD at non-zero density and temperature obtained from lattice calculations with almost physical quark masses for two values of the lattice cut-off $aT=1/4$ and 1/6 . We show that with our improved p4fa3-action the cut-off effects are under control when using lattices with a temporal extent of 6 or larger and that the contribution to the equation of state, which is due to a finite chemical potential is small for $\mu_q/T<1$. Moreover, at vanishing chemical potential, i.e. under conditions almost realized at RHIC and the LHC, quartic fluctuations of net baryon number and strangeness are large in a narrow temperature interval characterizing the transition region from the low to high temperature phase. At non-zero baryon number density, strangeness fluctuations are enhanced and correlated to fluctuations of the net baryon number. If strangeness is furthermore forced to vanish, as it may be the case in systems created in heavy ion collisions, strangeness fluctuations are significantly smaller than baryon number fluctuations.
Strangeness production at finite temperature and baryon density in an effective relativistic mean field model  [PDF]
F. Iazzi,R. Introzzi,A. Lavagno,D. Pigato,M. H. Younis
Physics , 2012, DOI: 10.1142/S0218301312500280
Abstract: We study the strangeness production in hot and dense nuclear medium, by requiring the conservation of the baryon density, electric charge fraction and zero net strangeness. The hadronic equation of state is investigated by means of an effective relativistic mean field model, with the inclusion of the full octet of baryons and kaon mesons. Kaons are considered taking into account of an effective chemical potential depending on the self-consistent interaction between baryons. The obtained results are compared with a minimal coupling scheme, calculated for different values of the anti-kaon optical potential and with non-interacting kaon particles. In this context, we also consider the possible onset of the kaon condensation for a wide range of temperatures and baryon densities.
Baryon Number and Electric Charge Fluctuations in Pb+Pb Collisions at SPS energies  [PDF]
V. P. Konchakovski,M. I. Gorenstein,E. L. Bratkovskaya,H. Stocker
Physics , 2006, DOI: 10.1103/PhysRevC.74.064911
Abstract: Event-by-event fluctuations of the net baryon number and electric charge in nucleus-nucleus collisions are studied in Pb+Pb at SPS energies within the HSD transport model. We reveal an important role of the fluctuations in the number of target nucleon participants. They strongly influence all measured fluctuations even in the samples of events with rather rigid centrality trigger. This fact can be used to check different scenarios of nucleus-nucleus collisions by measuring the multiplicity fluctuations as a function of collision centrality in fixed kinematical regions of the projectile and target hemispheres. The HSD results for the event-by-event fluctuations of electric charge in central Pb+Pb collisions at 20, 30, 40, 80 and 158 A GeV are in a good agreement with the NA49 experimental data and considerably larger than expected in a quark-gluon plasma. This demonstrate that the distortions of the initial fluctuations by the hadronization phase and, in particular, by the final resonance decays dominate the observable fluctuations.
On Fluctuations of Conserved Charges : Lattice Results Versus Hadron Resonance Gas  [PDF]
Pasi Huovinen,Peter Petreczky
Physics , 2010, DOI: 10.1088/1742-6596/230/1/012012
Abstract: We compare recent lattice results on fluctuations and correlations of strangeness, baryon number and electric charge obtained with p4 improved staggered action with the prediction of hadron resonance gas model. We show that hadron resonance gas can describe these fluctuations reasonably well if the hadron properties are as calculated on the lattice.
Charge, strangeness and radius of strangelets
Wen, X. J.;Peng, G. X.;Chen, Y. D.
High Energy Physics - Phenomenology , 2007, DOI: 10.1088/0954-3899/34/7/010
Abstract: We investigate, at both zero and finite temperature, the properties of strangelets versus the electric charge Z and strangeness S. The strangelet radius is not a monotonic function of either charge or strangeness, and a minimum is reached in the (Z, S) plane. However, the thermodynamically stable strangelets do not correspond to the radius minimum. The minimum radius always appears at positive strangeness, while the stable radius may appear at negative strangeness for very small baryon numbers. For large baryon numbers, the stable radius is proportional to the cubic root of baryon numbers, but inversely proportional to the square root of the confinement parameter in the present model. If bulk strange quark matter is absolutely stable, the reduced size of strangelets is about 1 fm, which may be relevant for the analysis of the strangelet production and detection.
Strangeness at high temperatures: from hadrons to quarks  [PDF]
A. Bazavov,H. -T. Ding,P. Hegde,O. Kaczmarek,F. Karsch,E. Laermann,Y. Maezawa,Swagato Mukherjee,H. Ohno,P. Petreczky,C. Schmidt,S. Sharma,W. Soeldner,M. Wagner
Physics , 2013, DOI: 10.1103/PhysRevLett.111.082301
Abstract: Appropriate combinations of up to fourth order cumulants of net strangeness fluctuations and their correlations with net baryon number and electric charge fluctuations, obtained from lattice QCD calculations, have been used to probe the strangeness carrying degrees of freedom at high temperatures. For temperatures up to the chiral crossover separate contributions of strange mesons and baryons can be well described by an uncorrelated gas of hadrons. Such a description breaks down in the chiral crossover region, suggesting that the deconfinement of strangeness takes place at the chiral crossover. On the other hand, the strangeness carrying degrees of freedom inside the quark gluon plasma can be described by a weakly interacting gas of quarks only for temperatures larger than twice the chiral crossover temperature. In the intermediate temperature window these observables show considerably richer structures, indicative of the strongly interacting nature of the quark gluon plasma.
Freeze-out parameters from electric charge and baryon number fluctuations: is there consistency?  [PDF]
S. Borsanyi,Z. Fodor,S. D. Katz,S. Krieg,C. Ratti,K. K. Szabo
Physics , 2014, DOI: 10.1103/PhysRevLett.113.052301
Abstract: Recent results for moments of multiplicity distributions of net-protons and net-electric charge from the STAR collaboration are compared to lattice QCD results for higher order fluctuations of baryon number and electric charge by the Wuppertal-Budapest collaboration, with the purpose of extracting the freeze-out temperature and chemical potential. All lattice simulations are performed for a system of 2+1 dynamical quark flavors, at the physical mass for light and strange quarks; all results are continuum extrapolated. We show that it is possible to extract an upper value for the freeze-out temperature, as well as precise baryo-chemical potential values corresponding to the four highest collision energies of the experimental beam energy scan. Consistency between the freeze-out parameters obtained from baryon number and electric charge fluctuations is found. The freeze-out chemical potentials are now in agreement with the statistical hadronization model.
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