Probing the softest region of nuclear equation of state

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dc.creatorLi, Bao-An
dc.creatorKo, C. M.
dc.date1998-07-31
dc.date.accessioned2026-07-07T11:11:48Z
dc.date.available2026-07-07T11:11:48Z
dc.descriptionAn attractive, energy-dependent mean-field potential for baryons is introduced in order to generate a soft region in the nuclear equation-of-state, as suggested by recent lattice QCD calculations of baryon free matter at finite temperature. Based on a hadronic transport model, we find that although this equation-of-state has negligible effects on the inclusive hadronic spectra, it leads to a minimum in the energy dependence of the transverse collective flow and a delayed expansion of the compressed matter. In particular, the transverse flow changes its direction as the colliding system passes through the softest region in the equation-of-state.
dc.description7 LaTex pages+4 figurs, Phy. Rev. C (1998) in press
dc.identifierhttps://arxiv.org/abs/nucl-th/9807088
dc.identifierhttp://arxiv.org/abs/nucl-th/9807088
dc.identifierPhys.Rev.C58:1382-1384,1998
dc.identifierdoi:10.1103/PhysRevC.58.1382
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/191220
dc.subjectNuclear Theory
dc.subjectNuclear Experiment
dc.titleProbing the softest region of nuclear equation of state
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