String dynamics in hadronic matter

Sorge, H.; Keitz, A. von; Mattiello, R.; Stöcker, H.; Greiner, Walter

doi:10.1007/bf01552329

Cited by 53 publications

(18 citation statements)

References 20 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…JAM results are similar to RQMD and UrQMD calculations [15,3]. Both constituent quark scattering [15,3] and diquark breaking [17,18] are important for the explanation of baryon stopping at SPS energies in hadronic cascade picture.…”

Section: Parton Cascade Vs Hadronic Cascadesupporting

confidence: 71%

Detailed comparison between parton cascade and hadronic cascade at SPS and RHIC

Nara¹,

Geiger²,

Longacre³

1999

AIP Conference Proceedings

View full text Add to dashboard Cite

For the STAR COLLABORATION aWhen the Relativistic Hei)wy Ion Collider (RHIC) at BNL begins operation in the Fall of 1999, heavy ions will be accelerated in collider mode for the first time, and a new energy regime will be entered for Heavy Ion Physics. The Solenoidal Tracker At RHIC (STAR) detector has a near 47r coverage and is dedicated to taking hadronic measuren]ents. A large volume Time Projection Chamber placed in a solenoidal magnet at 0.5T is used to track and identify the many thousands of produced particles. STiiR will measure many observable simultaneously on an event-by-event basis to study signatures of a possible QGP phase transition and the spsxe-time evolution of the collision process. The goal is to obtain a fundamental understanding of the microscopic structure of hadronic interactions, at the level of quarks and gluons, at high energy densities. This paper outlines the physics STAR intends to study during t] Ie first year of operation.

show abstract

Section: Parton Cascade Vs Hadronic Cascadesupporting

confidence: 71%

Detailed comparison between parton cascade and hadronic cascade at SPS and RHIC

Nara¹,

Geiger²,

Longacre³

1999

AIP Conference Proceedings

View full text Add to dashboard Cite

show abstract

“…In general, leading hadrons which contain original constituent quarks can scatter during their formation time with cross sections reduced according to the additive quark model. The importance of this quark(diquark)-hadron interaction for the description of baryon stopping at CERN/SPS energies has been reported by Frankfurt group [97,98,99,100,101].…”

Section: Hadronic Cascadementioning

confidence: 99%

“…In this work we use the microscopic transport model JAM [61,95] for that purpose. In JAM, the trajectories of all hadrons and resonances, including those produced in resonance or string decays, are propagated along their classical trajectories like in other microscopic hadronic transport models such as RQMD [96,97,98,99], and UrQMD [100,101,102]. To achieve a more sophisticated hadronic EoS, a mean field can be included within a framework of either Boltzmann-Uehling-Uhlenberck (BUU) model [103], or Quantum Molecular Dynamics (QMD) [104] approach.…”

Section: Hadronic Cascadementioning

confidence: 99%

See 1 more Smart Citation

Integrated dynamical approach to relativistic heavy ion collisions

Hirano

Huovinen

Murase

et al. 2013

Progress in Particle and Nuclear Physics

120

110

View full text Add to dashboard Cite

We review integrated dynamical approaches to describe heavy ion reaction as a whole at ultrarelativistic energies. Since final observables result from all the history of the reaction, it is important to describe all the stages of the reaction to obtain the properties of the quark gluon plasma from experimental data. As an example of these approaches, we develop an integrated dynamical model, which is composed of a fully (3+1) dimensional ideal hydrodynamic model with the state-of-the-art equation of state based on lattice QCD, and subsequent hadronic cascade in the late stage. Initial conditions are obtained employing Monte Carlo versions of the Kharzeev-LevinNardi model (MC-KLN) or the Glauber model (MC-Glauber). Using this integrated model, we first simulate relativistic heavy ion collisions at the RHIC and LHC energies starting from conventional smooth initial conditions. We next utilise each Monte Carlo samples of initial conditions on an event-by-event basis and perform event-by-event dynamical simulations to accumulate a large number of minimum bias events. A special attention is paid to performing the flow analysis as in experiments toward consistent comparison of theoretical results with experimental data.

show abstract

“…Still in the framework of conventional physics, the Relativistic Quantum Molecular Dynamical model, RQMD [14] -an extension of concepts previously applied to intermediate-energy nucleus-nucleus collisions -was recently proposed. It postulates the formation of "colour ropes" within a high string density.…”

Section: -E V Ent Generatorsmentioning

confidence: 99%

Charged-particle multiplicity and transverse energy measured in32S central interactions at 200 GeV per nucleon

Aoki

Bisi²,

Breslin

et al. 1995

Nuov Cim A

View full text Add to dashboard Cite

Abstract. -Interactions induced by 200 GeV per nucleon 32 S ions on heavy targets were selected by the HELIOS calorimeters and studied in nuclear emulsions. Global observables, such a s c harged particle multiplicity and transverse energy, w ere determined event-by-event. Multiplicity and transverse energy were measured as a function of the pseudorapidity o v er the large acceptance of the present experiment (0.6 5:5). A comparison of the experimental data with those provided by the event generators FRITIOF and VENUS shows remarkable dierences both in the target spectator region and in the participant region. An attempt is made to interpret these discrepancies in terms of plausible mechanisms, like baryon-pair production or rescattering.PACS 25.75 -Relativistic heavy-ion nuclear reactions. 1 1 -I n troduction.In the search for a transition from ordinary hadron matter to a deconned chiral-symmetric quark-gluon plasma (QGP), ultra-relativistic heavy-ion collisions have been extensively studied in the last few years [1]. The initial experimental activity, successfully dealing with huge hadronic showers, demonstrated that a high enough energy density, a prerequisite for deconnement, is attainable in central collisions. However signatures of a phase transition, previously anticipated as unambiguous, such a s J / suppression or strangeness enhancement, indeed observed, were put in question, revised and somehow incorporated in less exotic schemes [2]. On the other hand, both QCD lattice calculations dening the plasma phase and rst attempts to put forward a quark-gluon transport theory progressed slowly [3][4][5].Whereas experiments with beams of much heavier ions, now collecting data both at CERN and at BNL, will probably clarify at least some of the many open questions, it is worth comparing the available data with calculations based on conventional physics. In fact, at present, any mismatch b e t w een data and predictions could hardly be claimed as an unambiguous signal of a phase transition, but just shows that complex beam-target interactions cannot be treated as a superposition of independent n ucleon-nucleon collisions. At least, more realistic models of conventional physics should be attempted, taking benet from the amount and quality o f t h e a v ailable data.In this paper we present the analysis of a sample of interactions induced by 200 GeV per nucleon 32 S ions, selected by transverse energy, E T , and studied in nuclear emulsions. The accurate measurement on each e v ent o f b o t h c harged particle multiplicity and transverse energy is a unique feature of the present experiment. This work considerably improves our previous results [6], in particular due to the increased statistics and to the wider pseudorapidity range, now spanning from the target fragmentation region up to the projectile fragmentation region.2 -Experimental procedure.Nuclear emulsion stacks were exposed to a 200 GeV per nucleon 32 S beam in the target region of the HELIOS (High-Energy Lepton and IOn Spectrometer) apparatus at CERN [7,8...

show abstract

String dynamics in hadronic matter

Cited by 53 publications

References 20 publications

Detailed comparison between parton cascade and hadronic cascade at SPS and RHIC

Detailed comparison between parton cascade and hadronic cascade at SPS and RHIC

Integrated dynamical approach to relativistic heavy ion collisions

Charged-particle multiplicity and transverse energy measured in32S central interactions at 200 GeV per nucleon

Contact Info

Product

Resources

About