Isospin and isospin/strangeness correlations in relativistic heavy ion collisions

dc.creatorMekjian, Aram
dc.date2007-12-11
dc.date.accessioned2026-07-07T11:13:42Z
dc.date.available2026-07-07T11:13:42Z
dc.descriptionA fundamental symmetry of nuclear and particle physics is isospin whose third component is the Gell-Mann/Nishijima expression I(z)=Q-(B+S)/2 . The role of isospin symmetry in relativistic heavy ion collisions is studied. An isospin I(z), strangeness S correlation is shown to be a direct and simple measure of flavor correlations, vanishing in a Qg phase of uncorrelated flavors in both symmetric N=Z and asymmetric N not equal to Z systems. By contrast, in a hadron phase, a I(z)/S correlation exists as long as the electrostatic charge chemical potential mu(Q)does not equal 0 as in N not equal to Z asymmetric systems. A parallel is drawn with a Zeeman effect which breaks a spin degeneracy
dc.description11 pages
dc.identifierhttps://arxiv.org/abs/0712.1778
dc.identifierhttp://arxiv.org/abs/0712.1778
dc.identifierEur.Phys.J.80:22002,2007
dc.identifierdoi:10.1209/0295-5075/80/22002
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/191808
dc.subjectNuclear Theory
dc.titleIsospin and isospin/strangeness correlations in relativistic heavy ion collisions
dc.typetext

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