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Variation of the strange-quark chemical potential in the phase diagram of nuclear matter
On the basis of lattice calculations, we require the existence of a deconfined quark matter region (0<a/sub s/<1) beyond the hadron gas phase, which goes asymptotically into the ideal quark-gluon plasma domain, in the phase diagram of nuclear matter. We consider empirically the dynamics of thi...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2002
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/0954-3899/28/7/375 http://cds.cern.ch/record/593032 |
Sumario: | On the basis of lattice calculations, we require the existence of a deconfined quark matter region (0<a/sub s/<1) beyond the hadron gas phase, which goes asymptotically into the ideal quark-gluon plasma domain, in the phase diagram of nuclear matter. We consider empirically the dynamics of this region in terms of the order parameters and mass-scaled partition functions and derive an EoS. Then, the strange-quark chemical potential is expressed in a functional form of the temperature and light-quark chemical potential and its variation throughout the 3-region phase diagram is studied. We propose the change of the sign of the strange-quark chemical potential, from positive in the hadronic region to negative beyond, to be a unique, concise and well-defined indication of the quark- deconfinement phase transition in nuclear matter. Analysis of the nucleus-nucleus collision data from AGS and SPS is presented giving strong support to our proposal. (23 refs). |
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