Refine
Year of publication
Document Type
- Preprint (227) (remove)
Has Fulltext
- yes (227) (remove)
Is part of the Bibliography
- no (227)
Keywords
- Kollisionen schwerer Ionen (33)
- heavy ion collisions (27)
- Quark-Gluon-Plasma (14)
- equation of state (12)
- QGP (11)
- Quark Gluon Plasma (9)
- quark (9)
- quark-gluon plasma (9)
- Hadron (8)
- Zustandsgleichung (8)
- collision (8)
- heavy-ion collisions (8)
- Meson (7)
- heavy ion collision (7)
- meson (7)
- quark gluon plasma (7)
- Energie (6)
- Kollision (6)
- Quanten-Chromodynamik (6)
- Quark (6)
- UrQMD (6)
- LHC (5)
- MEMOs (5)
- QCD (5)
- Quantum Chromodynamic (5)
- RHIC (5)
- baryon (5)
- energy (5)
- hadronic (5)
- quark-gluon-plasma (5)
- relativistic (5)
- Dirac (4)
- Quark Materie (4)
- Relativistic heavy-ion collisions (4)
- SPS (4)
- hadron (4)
- heavy ion colliders (4)
- nucleon (4)
- quark matter (4)
- Bremsstrahlung (3)
- Molekulare Dynamik (3)
- Neutronenstern (3)
- Nukleon (3)
- RQMD (3)
- Strahl (3)
- Strangelets (3)
- Ultrarelativistic Quantum Molecular Dynamics (3)
- Zustandsgleichungen (3)
- black holes (3)
- bremsstrahlung (3)
- gluon (3)
- hadronic matter (3)
- hydrodynamical model (3)
- hydrodynamisches Modell (3)
- jet (3)
- kaon (3)
- neutron star (3)
- nuclear collisions (3)
- relativistic quantum molecular dynamics (3)
- relativistisch (3)
- schwere Ion Kollision (3)
- schwere Ion-Kollision (3)
- strangelets (3)
- CDM (2)
- Dichte (2)
- Dirac-Brueckner theory (2)
- Dirac-Brückner Theorie (2)
- Drell-Yan (2)
- Kaon (2)
- Kerne (2)
- Lagrangian (2)
- Materie (2)
- Meson production (2)
- Nambu Jona-Lasinio Modell (2)
- Nambu Jona-Lasinio model (2)
- Partikelspektren (2)
- Phasenübergang (2)
- Plasma (2)
- QMD (2)
- Quanten Chromodynamik (2)
- Quantenchromodynamik (2)
- Quantum Chromodynamics (2)
- Quantum Molecular Dynamics (2)
- Quark gluon Plasma (2)
- Quark-Gluon Plasma (2)
- Teilchen (2)
- Temperatur (2)
- UrQMD Modell (2)
- Walecka model (2)
- antibaryon (2)
- antikaon (2)
- bound state (2)
- cold dark matter (2)
- degrees of freedom (2)
- dense matter (2)
- dichte Materie (2)
- freeze out (2)
- große Extradimensionen (2)
- hadronische Materie (2)
- kalte dunkle Materie (2)
- kinetic equation (2)
- kinetische Gleichung (2)
- large extra dimensions (2)
- masse (2)
- matter (2)
- neutralino (2)
- nuclear broadening effect (2)
- nuclear matter (2)
- nuclei (2)
- particle spectra (2)
- particles (2)
- plasma (2)
- prompt photon (2)
- relativistic heavy ion collision (2)
- relativistische schwere Ion Kollision (2)
- schwarze Löcher (2)
- schwere Ion-Kollisionen (2)
- statistical coalescence model (2)
- statistisches Fusionsmodell (2)
- strange hadronic matter (2)
- temperature (2)
- thermalization (2)
- ultrarelativistisch (2)
- ultrarelativistische (2)
- (QGP) (1)
- AGS (1)
- Absorption (1)
- Anisotropic flow (1)
- Anti-Kaon (1)
- Antikaon (1)
- Antiteilchen (1)
- Ausfrieren (1)
- Baryon (1)
- Bjorken Modell (1)
- Bjorken model (1)
- Boltzmann-Uehling-Uhlenbeck (1)
- Boltzmann-Uehling-Uhlenbeck Gleichung (1)
- Boltzmann-Uehling-Uhlenbeck equation (1)
- Charm Produktion (1)
- Charmed mesons (1)
- Charmed quarks (1)
- Charmonium (1)
- Charmonium Produktion (1)
- Charmonium production (1)
- Chemical equilibration (1)
- Chemikalie (1)
- Chemische Gleichgewichtherstellung (1)
- Chiral symmetries (1)
- Cluster distribution (1)
- Cluster integrals (1)
- Collision (1)
- Conservation Laws (1)
- D-Dbar (1)
- D-meson spectral density (1)
- DN interaction (1)
- Deuteron (1)
- Dielectron (1)
- Dielektron (1)
- Dilepton (1)
- Drell-Yan production (1)
- Drell-Yan ratio (1)
- Drell-Yan-Prozess (1)
- Dynamik (1)
- Dyson-Schwinger equation (1)
- EOS (1)
- Elektron (1)
- Elementarteilchen (1)
- Elementary particle (1)
- Equation of State (1)
- Ereignisschwankungen (1)
- Erhaltungsgesetz (1)
- Event-by-event fluctuations (1)
- Freeze Out (1)
- Freeze out (1)
- Freiheitsgrad (1)
- Freiheitsgrade (1)
- Gluon (1)
- Gluon-Plasma (1)
- Gyromagnetic Moment (1)
- HICs (1)
- Hadron Gas Modell (1)
- Hadron Materie (1)
- Hadronenbeschleuniger (1)
- Hartree (1)
- Heavy ion collisions (1)
- High Energy Physics - Phenomenology (1)
- Hohe Energie (1)
- Homogeneous nucleation (1)
- Hypermaterie (1)
- IQMD Modell (1)
- IQMD model (1)
- In-Medium Zerfall (1)
- J/psi Erhöhung (1)
- J/psi Unterdrückung (1)
- J/psi enhancement (1)
- J/psi suppression (1)
- J/psi yield (1)
- J/ϕ (1)
- K-Meson (1)
- Kaons (1)
- Kern-Kern Kollision (1)
- Kernkollision (1)
- Kernkollisionen (1)
- Kernmaterie (1)
- Kernreaktion Modell und Methoden (1)
- Kollisionen des schweren Ions (1)
- Kollisionen schwere Ionen (1)
- Korrelation (1)
- Kosmischer Strahl (1)
- Lagrangian . equation of state (1)
- Lambda-c(2593) resonance (1)
- Large Hadron Collider (1)
- Lorentz (1)
- Lorentz contraction (1)
- Mach Shocks (1)
- Masse (1)
- Massenspektrum (1)
- Metastable Exotic Multistrange Objects (1)
- Modell (1)
- Monte-Carlo model for relativistic heavy ion collisions (1)
- Nambu Jona Lasinio Modell (1)
- Nambu Jona Lasinio model (1)
- Nambu-Jona-Lasinio (1)
- Nambu-Jona-Lasinio Modell (1)
- Nambu-Jona-Lasinio model (1)
- Neutron (1)
- Nichtumkehrbarkeit (1)
- Nuclear Theory (1)
- Nuclear-reaction models and methods (1)
- Nucleon (1)
- OMD (1)
- Particle Spectra (1)
- Partikelzahlschwankung (1)
- Pb+Pb collisions (1)
- Photon (1)
- Pion (1)
- Pion Gas (1)
- Potential (1)
- Produktion von pentaquark (1)
- Protonen (1)
- QCD medium (1)
- QCD plasma (1)
- QGP hadrons phase transition (1)
- QGP signals (1)
- QMC (1)
- Quanten Chromodynamic (1)
- Quanten-Molekular-Dynamic (1)
- Quanten-Molekular-Dynamik (1)
- Quantendynamik (1)
- Quantum chromodynamics (1)
- Quark Antiquark (1)
- Quark-Sterne (1)
- Quarkonium (1)
- RHIC energies (1)
- Raum Zeit (1)
- Relativistic Excluded Volumes (1)
- Relativistic Heavy Ion Collider (1)
- Relativistisch (1)
- Relativistische Kollisionen des schwere Ions (1)
- Rho-Meson (1)
- SENECA model (1)
- SHM (1)
- SU (3) - Modell (1)
- SU (3) - Symmetrie (1)
- SU (3) Modell (1)
- SU(3) model (1)
- SU(3)-model (1)
- SU(3)-symmetry (1)
- Schwerionenphysik (1)
- Skalarpotential (1)
- Spektren (1)
- Statistical model (1)
- Super Proton Synchrotron (1)
- Symmetrie (1)
- Teilchenbeschleuniger (1)
- Teilchenspektren (1)
- Teilchenverteilung (1)
- Tevatron (1)
- Transport (1)
- Two-component and Multi-component Hadron Gas (1)
- URQMD (1)
- Ultra-relativistic Quantum Molecular Dynamic (1)
- Ultra-relativistic Quantum Molecular Dynamics model (1)
- Ultrarelativisitic Quantum Molecular Dynamics model (1)
- Ultrarelativisitisches (1)
- Ultrarelativistic Quantum Molecular Model (1)
- Ultrarelativistisches Quant Molekular Dynamik (1)
- Ultrarelativistisches Quant Molekulares Modell (1)
- UrQMD model (1)
- Van der Waals (1)
- Van der Waals Excluded Volume Model (1)
- Van der Waals model (1)
- Vektorpotential (1)
- Verbreitung (1)
- Vielkörperkorrelationen (1)
- Walecka Modell (1)
- Walecka-Modell (1)
- Walecka-model (1)
- Zusammenstoß (1)
- absorption (1)
- anti-kaon (1)
- antiparticles (1)
- black hole (1)
- broadening (1)
- charm (1)
- charm and bottom Produktion (1)
- charm and bottom production (1)
- chemical (1)
- chemical freezeout (1)
- chemisches Ausfrieren (1)
- chiral (1)
- chiral SU (3) (1)
- chiral SU(3) (1)
- chiral SU(3) model (1)
- chiral phase (1)
- cold baryon rich matter (1)
- cold quark matter (1)
- collective flow (1)
- color current (1)
- coloured quark dynamic (1)
- conservation law (1)
- conservation laws (1)
- coupled-channel self-consistent calculation (1)
- dense (1)
- density perturbations (1)
- deuteron (1)
- dilepton (1)
- dileptons (1)
- directed flow (1)
- electron (1)
- elliptic flow analysis (1)
- energie (1)
- exotic matter (1)
- exotische Materie (1)
- femtoscopy data (1)
- finite temperature (1)
- flow (1)
- flow of nucleons (1)
- freezeout (1)
- gluon plasma (1)
- großer hadron collider (1)
- gyromagnetic moment (1)
- hadron hadron Kollision (1)
- hadron hadron collision (1)
- hadron interaction models (1)
- hadron matter (1)
- hadron yield (1)
- hadronic freeze-out (1)
- hadronic model (1)
- hard-core (1)
- heavy Hagedorn states (1)
- heavy ion (1)
- heavy-flavor quarks (1)
- heiße Kernmaterie (1)
- heiße Materie (1)
- heiße Pion Materie (1)
- heiße hadronic Materie (1)
- heiße und dichte Kernmaterie (1)
- heiße und dichte Materie (1)
- hidden charm production (1)
- high energie (1)
- high energy (1)
- high energy cosmic ray (1)
- high-energy nuclear collisions (1)
- hitze (1)
- hohe Energie (1)
- homogene Nukleation (1)
- hot (1)
- hot and dense matter (1)
- hot and dense nuclear matter (1)
- hot hadronic matter (1)
- hot hypernuclear matter (1)
- hot matter (1)
- hot pion matter (1)
- hybrid approach to air shower simulations (1)
- hydrodynamics (1)
- hypermatter (1)
- hyperonic Materie (1)
- hyperonic matter (1)
- ideal gas (1)
- ideales Gas (1)
- in-medium decay (1)
- in-medium properties (1)
- irreversibility state (1)
- kaons (1)
- kinetisches Ausfrieren (1)
- kinetisches Modell (1)
- kollektive strom (1)
- kollidieren (1)
- lange hadron collider (1)
- large hadron collider (1)
- low energy hadronic model (1)
- many-body correlations (1)
- mass spectra (1)
- meson mass (1)
- microscopic transport theory (1)
- mikroskopische Transporttheorie (1)
- minimal length (1)
- minimale Länge (1)
- mixing of hadron sources (1)
- muon (1)
- neutron and proton chemical potential (1)
- non-equilibrium dynamics (1)
- non-equilibrium quantum field dynamics (1)
- nuclear (1)
- nuclear shadowing (1)
- nuclear system (1)
- nucleus-nucleus collisions (1)
- offene charm Produktion (1)
- open and hidden charm (1)
- open and hidden charm production (1)
- open charm production (1)
- open charm yield (1)
- pQCD (1)
- particle distribution (1)
- particle number fluctuations (1)
- particle ratios (1)
- partonic (1)
- perturbative Quantum Chromodynamic (1)
- phase transition (1)
- photon (1)
- pion (1)
- pion gas (1)
- pions (1)
- production of pentaquark (1)
- quark antiquark (1)
- quark gluon Plasma (1)
- quark-meson coupling model (1)
- quarkonium (1)
- reich (1)
- relativistic fluid of quarks (1)
- relativistic heavy ion collider (1)
- relativistischer Schwerionen-Zusammenstoßer (1)
- rho meson (1)
- rich (1)
- scalar potential (1)
- schwarzes Loch (1)
- schwere Hagedorn Zustände (1)
- schwere Ione (1)
- schwere Ionen Kollision (1)
- schweres Ion (1)
- second cluster integral (1)
- space-momentum correlation (1)
- space-time (1)
- spectra (1)
- stabile kalte Kerne (1)
- stable cold nuclear matter (1)
- strange (1)
- strange quark star (1)
- strangeness (1)
- superheavy (1)
- superheavy nuclei (1)
- superschwer (1)
- superschwere Kerne (1)
- supersymmetric particle (1)
- symmetry potential (1)
- system (1)
- thermal (1)
- transport models (1)
- ultra-relativistic heavy ion collision (1)
- ultrarelativistic (1)
- ultrarelativistic energie (1)
- ultrarelativistic heavy ion collision (1)
- ultrarelativistic heavy-ion collision (1)
- ultrarelativistische Kollision des schweren Ionen (1)
- ultrarelativistische energie (1)
- ultrarelativistische schwere Ion Kollision (1)
- van der Waals (1)
- vector mesons (1)
- vector potential (1)
- zweite Gruppenintegral (1)
Institute
In the framework of RQMD we investigate antiproton observables in massive heavy ion collisions at AGS energies and compare to preliminary results of the E878 collaboration. We focus here on the considerable influence of the real part of an antinucleon nucleus optical potential on the ¯p momentum spectra. Pacs-numbers: 14.20 Dh, 25.70.-z
Spectra of various particle species have been calculated with the Quantum Molecular Dynamics (QMD) model for very central collisions of Au+Au. They are compatible with the idea of a fully stopped thermal source which exhibits a transversal expansion besides the thermal distribution of an ideal gas. How- ever, the microscopic analyses of the local flow velocities and temperatures indicate much lower temperatures at densities associated with the freeze-out. The results express the overall impossibility of a model-independent determi- nation of nuclear temperatures from heavy ion spectral data, also at other energies (e.g. CERN) or for other species (i.e. pions, kaons, hyperons)
In the framework of the relativistic quantum molecular dynamics approach (RQMD) we investigate antideuteron (d) observables in Au+Au collisions at 10.7 AGeV. The impact parameter dependence of the formation ratios d/p2 and d/p2 is calculated. In central collisions, the antideuteron formation ratio is predicted to be two orders of magnitude lower than the deuteron formation ratio. The d yield in central Au+Au collisions is one order of magnitude lower than in Si+Al collisions. In semicentral collisions di erent configuration space distributions of p s and d s lead to a large squeeze out e ect for antideuterons, which is not predicted for the p s.
We predict the formation of highly dense baryon-rich resonance matter in Au+Au collisions at AGS energies. The final pion yields show observable signs for resonance matter. The Delta1232 resonance is predicted to be the dominant source for pions of small transverse momenta. Rescattering e ects consecutive excitation and deexcitation of Delta's lead to a long apparent life- time (> 10 fm/c) and rather large volumina (several 100 fm3) of the Delta-matter state. Heavier baryon resonances prove to be crucial for reaction dynamics and particle production at AGS.
We calculate thermal photon and neutral pion spectra in ultrarelativistic heavy-ion collisions in the framework of three-fluid hydrodynamics. Both spectra are quite sensitive to the equation of state used. In particular, within our model, recent data for S + Au at 200 AGeV can only be understood if a scenario with a phase transition (possibly to a quark-gluon plasma) is assumed. Results for Au+Au at 11 AGeV and Pb + Pb at 160 AGeV are also presented.
We develop a 1+1 dimensional hydrodynamical model for central heavy-ion collisions at ultrarelativistic energies. Deviations from Bjorken's scaling are taken into account by implementing finite-size profiles for the initial energy density. The calculated rapidity distributions of pions, kaons and antiprotons in central Au+Au collisions at the c.m. energy 200 AGeV are compared with experimental data of the BRAHMS Collaboration. The sensitivity of the results to the choice of the equation of state, the parameters of initial state and the freeze-out conditions is investigated. The best fit of experimental data is obtained for a soft equation of state and Gaussian-like initial profiles of the energy density.
The concept of Large Extra Dimensions (LED) provides a way of solving the Hierarchy Problem which concerns the weakness of gravity compared with the strong and electro-weak forces. A consequence of LED is that miniature Black Holes (mini-BHs) may be produced at the Large Hadron Collider in p+p collisions. The present work uses the CHARYBDIS mini-BH generator code to simulate the hadronic signal which might be expected in a mid-rapidity particle tracking detector from the decay of these exotic objects if indeed they are produced. An estimate is also given for Pb+Pb collisions.
The experimental signatures of TeV-mass black hole (BH) formation in heavy ion collisions at the LHC is examined. We find that the black hole production results in a complete disappearance of all very high p_T (> 500 GeV) back-to-back correlated di-jets of total mass M > M_f ~ 1 TeV. We show that the subsequent Hawking-decay produces multiple hard mono-jets and discuss their detection. We study the possibility of cold black hole remnant (BHR) formation of mass ~ M_f and the experimental distinguishability of scenarios with BHRs and those with complete black hole decay. Due to the rather moderate luminosity in the first year of LHC running the least chance for the observation of BHs or BHRs at this early stage will be by ionizing tracks in the ALICE TPC. Finally we point out that stable BHRs would be interesting candidates for energy production by conversion of mass to Hawking radiation.
We examine experimental signatures of TeV-mass black hole formation in heavy ion collisions at the LHC. We find that the black hole production results in a complete disappearance of all very high p_T (> 500 GeV) back-to-back correlated di-jets of total mass M > M_f ~ 1 TeV. We show that the subsequent Hawking-decay produces multiple hard mono-jets and discuss their detection. We study the possibility of cold black hole remnant (BHR) formation of mass ~ M_f and the experimental distinguishability of scenarios with BHRs and those with complete black hole decay. Finally we point out that a Heckler-Kapusta-Hawking plasma may form from the emitted mono-jets. In this context we present new simulation data of Mach shocks and of the evolution of initial conditions until the freeze-out.
The production of Large Extra Dimension (LXD) Black Holes (BHs), with a new, fundamental mass scale of M_f = 1 TeV, has been predicted to occur at the Large Hadron Collider, LHC, with the formidable rate of 10^8 per year in p-p collisions at full energy, 14 TeV, and at full luminosity. We show that such LXD-BH formation will be experimentally observable at the LHC by the complete disappearance of all very high p_t (> 500 GeV) back-to-back correlated Di-Jets of total mass M > M_f = 1 TeV. We suggest to complement this clear cut-off signal at M > 2*500 GeV in the di-jet-correlation function by detecting the subsequent, Hawking-decay products of the LXD-BHs, namely either multiple high energy (> 100 GeV) SM Mono-Jets (i.e. away-side jet missing), sprayed off the evaporating BHs isentropically into all directions or the thermalization of the multiple overlapping Hawking-radiation in a eckler-Kapusta-Plasma. Microcanonical quantum statistical calculations of the Hawking evaporation process for these LXD-BHs show that cold black hole remnants (BHRs) of Mass sim M_f remain leftover as the ashes of these spectacular Di-Jet-suppressed events. Strong Di-Jet suppression is also expected with Heavy Ion beams at the LHC, due to Quark-Gluon-Plasma induced jet attenuation at medium to low jet energies, p_t < 200 GeV. The (Mono-)Jets in these events can be used to trigger for Tsunami-emission of secondary compressed QCD-matter at well defined Mach-angles, both at the trigger side and at the awayside (missing) jet. The Machshock-angles allow for a direct measurement of both the equation of state EoS and the speed of sound c_s via supersonic bang in the "big bang" matter. We discuss the importance of the underlying strong collective flow - the gluon storm - of the QCD- matter for the formation and evolution of these Machshock cones. We predict a significant deformation of Mach shocks from the gluon storm in central Au+Au collisions at RHIC and LHC energies, as compared to the case of weakly coupled jets propagating through a static medium. A possible complete stopping of pt > 50 GeV jets at the LHC in 2-3 fm yields nonlinear high density Mach shocks in he quark gluon plasma, which can be studied in the complex emission and disintegration pattern of the possibly supercooled matter. We report on first full 3-dimensional fluid dynamical studies of the strong effects of a first order phase transition on the evolution and the Tsunami-like Mach shock emission of the QCD matter.
We have calculated the D-meson spectral density at finite temperature within a self-consistent coupled-channel approach that generates dynamically the Lambda_c (2593) resonance. We find a small mass shift for the D-meson in this hot and dense medium while the spectral density develops a sizeable width. The reduced attraction felt by the D-meson in hot and dense matter together with the large width observed have important consequences for the D-meson production in the future CBM experiment at FAIR.
The rapidity dependence of the single- and double- neutron to proton ratios of nucleon emission from isospin-asymmetric but mass-symmetric reactions Zr+Ru and Ru+Zr at energy range 100 ~ 800 A MeV and impact parameter range 0 ~ 8 fm is investigated. The reaction system with isospin-asymmetry and mass-symmetry has the advantage of simultaneously showing up the dependence on the symmetry energy and the degree of the isospin equilibrium. We find that the beam energy- and the impact parameter dependence of the slope parameter of the double neutron to proton ratio (F_D) as function of rapidity are quite sensitive to the density dependence of symmetry energy, especially at energies E_b ~ 400 A MeV and reduced impact parameters around 0.5. Here the symmetry energy effect on the F_D is enhanced, as compared to the single neutron to proton ratio. The degree of the equilibrium with respect to isospin (isospin mixing) in terms of the F_D is addressed and its dependence on the symmetry energy is also discussed.
Several observables of unbound nucleons which are to some extent sensitive to the medium modifications of nucleon-nucleon elastic cross sections in neutron-rich intermediate energy heavy ion collisions are investigated. The splitting effect of neutron and proton effective masses on cross sections is discussed. It is found that the transverse flow as a function of rapidity, the Q_zz as a function of momentum, and the ratio of halfwidths of the transverse to that of longitudinal rapidity distribution R_t/l are very sensitive to the medium modifications of the cross sections. The transverse momentum distribution of correlation functions of two-nucleons does not yield information on the in-medium cross section.
The pion source as seen through HBT correlations at RHIC energies is investigated within the UrQMD approach. We find that the calculated transverse momentum, centrality, and system size dependence of the Pratt-HBT radii R_L and R_S are reasonably well in line with experimental data. The predicted R_O values in central heavy ion collisions are larger as compared to experimental data. The corresponding quantity sqrt R_O^2-R_S^2 of the pion emission source is somewhat larger than experimental estimates.
Using a microscopic transport model together with a coalescence after-burner, we study the formation of deuterons in Au + Au central collisions at s = 200 AGeV . It is found that the deuteron transverse momentum distributions are strongly a ected by the nucleon space-momentum correlations, at the moment of freeze-out, which are mostly determined by the number of rescatterings. This feature is useful for studying collision dynamics at ultrarelativistic energies.
Elliptic flow analysis at RHIC with the Lee-Yang Zeroes method in a relativistic transport approach
(2006)
The Lee-Yang zeroes method is applied to study elliptic flow (v_2) in Au+Au collisions at sqrt s =200 A GeV, with the UrQMD model. In this transport approach, the true event plane is known and both the nonflow effects and event-by-event v_2 fluctuations exist. Although the low resolutions prohibit the application of the method for most central and peripheral collisions, the integral and differential elliptic flow from the Lee-Yang zeroes method agrees with the exact v_2 values very well for semi-central collisions.
The transverse momentum dependence of the anisotropic flow v_2 for pi, K, nucleon, Lambda, Xi and Omega is studied for Au+Au collisions at sqrt s_NN = 200 GeV within two independent string-hadron transport approaches (RQMD and UrQMD). Although both models reach only 60% of the absolute magnitude of the measured v_2, they both predict the particle type dependence of v_2, as observed by the RHIC experiments: v_2 exhibits a hadron-mass hierarchy (HMH) in the low p_T region and a number-of-constituent-quark (NCQ) dependence in the intermediate p_T region. The failure of the hadronic models to reproduce the absolute magnitude of the observed v_2 indicates that transport calculations of heavy ion collisions at RHIC must incorporate interactions among quarks and gluons in the early, hot and dense phase. The presence of an NCQ scaling in the string-hadron model results suggests that the particle-type dependencies observed in heavy-ion collisions at intermediate p_T are related to the hadronic cross sections in vacuum rather than to the hadronization process itself, as suggested by quark recombination models.
Based on the UrQMD transport model, the transverse momentum and the rapidity dependence of the Hanbury-Brown-Twiss (HBT) radii R_L, R_O, R_S as well as the cross term R_OL at SPS energies are investigated and compared with the experimental NA49 and CERES data. The rapidity dependence of the R_L, R_O, R_S is weak while the R_OL is significantly increased at large rapidities and small transverse momenta. The HBT "life-time" issue (the phenomenon that the calculated sqrt R_O^2-R_S^2 value is larger than the correspondingly extracted experimental data) is also present at SPS energies.
The cumulant method is applied to study elliptic flow (v_2) in Au+Au collisions at sqrt s=200 AGeV, with the UrQMD model. In this approach, the true event plane is known and both the non-flow effects and event-by-event spatial (epsilon) and v_2 fluctuations exist. Qualitatively, the hierarchy of v_2 's from two, four and six-particle cumulants is consistent with the STAR data, however, the magnitude of v_2 in the UrQMD model is only 60% of the data. We find that the four and six-particle cumulants are good measures of the real elliptic flow over a wide range of centralities except for the most central and very peripheral events. There the cumulant method is affected by the v_2 fluctuations. In mid-central collisions, the four and six-particle cumulants are shown to give a good estimation of the true differential v_2, especially at large transverse momentum, where the two-particle cumulant method is heavily affected by the non-flow effects.
We propose to measure correlations of heavy-flavor hadrons to address the status of thermalization at the partonic stage of light quarks and gluons in high-energy nuclear collisions, shown on the example of azimuthal correlations of D-Dbar pairs. We show that hadronic interactions at the late stage can not disturb these correlations significantly. Thus, a decrease or the complete absence of these initial correlations indicates frequent interactions of heavy-flavor quarks in the partonic stage. Therefore, early thermalization of light quarks is likely to be reached. PACS numbers: 25.75.-q
We propose to measure azimuthal correlations of heavy-flavor hadrons to address the status of thermalization at the partonic stage of light quarks and gluons in high-energy nuclear collisions. In particular, we show that hadronic interactions at the late stage cannot significantly disturb the initial back-to-back azimuthal correlations of DDbar pairs. Thus, a decrease or the complete absence of these initial correlations does indicate frequent interactions of heavy-flavor quarks and also light partons in the partonic stage, which are essential for the early thermalization of light partons.
To be published in J. Phys. G - Proceedings of SQM 2004 : We review the results from the various hydrodynamical and transport models on the collective flow observables from AGS to RHIC energies. A critical discussion of the present status of the CERN experiments on hadron collective flow is given. We emphasize the importance of the flow excitation function from 1 to 50 A.GeV: here the hydrodynamic model has predicted the collapse of the v2-flow ~ 10 A.GeV; at 40 A.GeV it has been recently observed by the NA49 collaboration. Since hadronic rescattering models predict much larger flow than observed at this energy we interpret this observation as evidence for a first order phase transition at high baryon density r b. Moreover, the connection of the elliptic flow v2 to jet suppression is examined. It is proven experimentally that the collective flow is not faked by minijet fragmentation. Additionally, detailed transport studies show that the away-side jet suppression can only partially (< 50%) be due to hadronic rescattering. Furthermore, the change in sign of v1, v2 closer to beam rapidity is related to the occurence of a high density first order phase transition in the RHIC data at 62.5, 130 and 200 A.GeV.
Bounding Dark Energy from the SPARC rotation curves: Data driven probe for galaxy virialization
(2024)
Dark Energy (DE) acts as a repulsive force that opposes gravitational attraction. Assuming galaxies maintain a steady state over extended periods, the estimated upper bound on DE studies its resistance to the attractive gravitational force from dark matter. Using the SPARC dataset, we fit the Navarro-Frenk-White (NFW) and Hernquist models to identify the most suitable galaxies for these models. Introducing the presence of DE in these galaxies helps establish the upper limit on its repulsive force. This upper bound on DE sits around ρ(<Λ)∼10−25~kg/m3, only two orders of magnitude higher than the one measured by Planck. We discuss the conditions for detecting DE in different systems and show the consistency of the upper bound from galaxies to other systems. The upper bound is of the same order of magnitude as ρ200=200ρc for both dark matter profiles. We also address the implications for future measurements on that upper bound and the condition for detecting the impact of Λ on galactic scales.
Gravitational waves from a core g-mode in supernovae as probes of the high-density equation of state
(2023)
Using relativistic supernova simulations of massive progenitor stars with a quark-hadron equation of state (EoS) and a purely hadronic EoS, we identify a distinctive feature in the gravitational-wave signal that originates from a buoyancy-driven mode (g-mode) below the proto-neutron star convection zone. The mode frequency lies in the range 200≲f≲800Hz and decreases with time. As the mode lives in the core of the proto-neutron star, its frequency and power are highly sensitive to the EoS, in particular the sound speed around twice saturation density.
Gravitational waves from a core g-mode in supernovae as probes of the high-density equation of state
(2023)
Using relativistic supernova simulations of massive progenitor stars with a quark-hadron equation of state (EoS) and a purely hadronic EoS, we identify a distinctive feature in the gravitational-wave signal that originates from a buoyancy-driven mode (g-mode) below the proto-neutron star convection zone. The mode frequency lies in the range 200≲f≲800Hz and decreases with time. As the mode lives in the core of the proto-neutron star, its frequency and power are highly sensitive to the EoS, in particular the sound speed around twice saturation density.