dorsal/arxiv
View SchemaTwo Phase Simulation of Ultrarelativistic Nuclear Collisions
| Authors | D. E. Kahana, S. H. Kahana |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/9804017 |
| URL | https://arxiv.org/abs/nucl-th/9804017 |
| DOI | 10.1103/PhysRevC.58.3574 |
| Journal | Phys.Rev.C58:3574-3586,1998 |
Abstract
A two phase cascade is presented for the treatment of ultra-high energy ion-ion collisions at energies from 17-200 GeV. First a high energy, fast cascade is performed, in which original baryons and freed hard partons, if any, collide. This stage ignores energy loss from soft (slow) processes. In this first version no hard processes, aside from Drell-Yan production, are included. The space-time history of the hard phase is then used as input to reconstruct soft energy-loss, which occurs over a longer time scale. Soft meson production is therefore treated as coherent over groups of interacting nucleons. Two body data, though, are used extensively to guide the reinitialisation of the cascade, which satisfies conservation laws for charge, strangeness and of course, energy-momentum. A second phase, low energy cascade is finally carried out among the products of the hard cascade. The model selected to describe elementary hadron-hadron collisions in the soft cascade incorporates generic mesons and baryons, which are the agents for rescattering. We imagine a constituent quark model applies, with generic mesons consisting of an excited quark-antiquark pair, and generic baryons constructed from three quarks. The chief result is a reconciliation of the important Drell-Yan measurements, indicating high-mass lepton pairs are produced as if no energy is lost from the nucleons, with the apparent success of a purely hadronic, soft cascade in describing nucleon stopping and meson production in heavy ion experiments at the CERN SPS.
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"abstract": "A two phase cascade is presented for the treatment of ultra-high energy\nion-ion collisions at energies from 17-200 GeV. First a high energy, fast\ncascade is performed, in which original baryons and freed hard partons, if any,\ncollide. This stage ignores energy loss from soft (slow) processes. In this\nfirst version no hard processes, aside from Drell-Yan production, are included.\nThe space-time history of the hard phase is then used as input to reconstruct\nsoft energy-loss, which occurs over a longer time scale. Soft meson production\nis therefore treated as coherent over groups of interacting nucleons. Two body\ndata, though, are used extensively to guide the reinitialisation of the\ncascade, which satisfies conservation laws for charge, strangeness and of\ncourse, energy-momentum. A second phase, low energy cascade is finally carried\nout among the products of the hard cascade. The model selected to describe\nelementary hadron-hadron collisions in the soft cascade incorporates generic\nmesons and baryons, which are the agents for rescattering. We imagine a\nconstituent quark model applies, with generic mesons consisting of an excited\nquark-antiquark pair, and generic baryons constructed from three quarks. The\nchief result is a reconciliation of the important Drell-Yan measurements,\nindicating high-mass lepton pairs are produced as if no energy is lost from the\nnucleons, with the apparent success of a purely hadronic, soft cascade in\ndescribing nucleon stopping and meson production in heavy ion experiments at\nthe CERN SPS.",
"arxiv_id": "nucl-th/9804017",
"authors": [
"D. E. Kahana",
"S. H. Kahana"
],
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"doi": "10.1103/PhysRevC.58.3574",
"journal_ref": "Phys.Rev.C58:3574-3586,1998",
"title": "Two Phase Simulation of Ultrarelativistic Nuclear Collisions",
"url": "https://arxiv.org/abs/nucl-th/9804017"
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