Evidence for nuclear matter with the highest baryon density in heavy-ion collisions between 3A and 10A GeV

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Abstract

We present a systematic comparison of the phase-space density of protons at the center-of-mass deduced from the available experimental data from 1A to 158A GeV. Nuclear matter with the highest baryon density can be obtained at a beam energy between 3A and 10A GeV, which is also supported by the beam-energy dependence of the transverse flow velocity at the center-of-mass. A search for Quantum Chromodynamical phase transitions in the high baryon-density region at a relatively low temperature should be performed at the Heavy-Ion Synchrotron (SIS) and at the Alternate Gradient Synchrotron (AGS).

Original languageEnglish
JournalJournal of the Korean Physical Society
Volume36
Issue number3
Publication statusPublished - 2000 Mar 1

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ionic collisions
center of mass
baryons
synchrotrons
space density
heavy ions
flow velocity
gradients
protons
energy

ASJC Scopus subject areas

  • Physics and Astronomy(all)

Cite this

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abstract = "We present a systematic comparison of the phase-space density of protons at the center-of-mass deduced from the available experimental data from 1A to 158A GeV. Nuclear matter with the highest baryon density can be obtained at a beam energy between 3A and 10A GeV, which is also supported by the beam-energy dependence of the transverse flow velocity at the center-of-mass. A search for Quantum Chromodynamical phase transitions in the high baryon-density region at a relatively low temperature should be performed at the Heavy-Ion Synchrotron (SIS) and at the Alternate Gradient Synchrotron (AGS).",
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AB - We present a systematic comparison of the phase-space density of protons at the center-of-mass deduced from the available experimental data from 1A to 158A GeV. Nuclear matter with the highest baryon density can be obtained at a beam energy between 3A and 10A GeV, which is also supported by the beam-energy dependence of the transverse flow velocity at the center-of-mass. A search for Quantum Chromodynamical phase transitions in the high baryon-density region at a relatively low temperature should be performed at the Heavy-Ion Synchrotron (SIS) and at the Alternate Gradient Synchrotron (AGS).

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