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The composition of the neutron star core for neutrino free matter, without (solid lines) and with (dashed lines) hyperons, for = 5 MeV (upper panel) and = 50 MeV (lower panel).

The composition of the neutron star core for neutrino free matter, without (solid lines) and with (dashed lines) hyperons, for = 5 MeV (upper panel) and = 50 MeV (lower panel).

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The FSU2H equation of state model, originally developed to describe cold neutron star matter with hyperonic cores, is extended to finite temperature. Results are presented for a wide range of temperatures and lepton fractions, which cover the conditions met in protoneutron star matter, neutron star mergers and supernova explosions. It is found that...

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Context 1
... this subsection we show the composition of the star for the abovementioned different cases. In Figure 1 the composition of a neutrino free neutron star core is shown for temperatures = 5 MeV (upper panel) and = 50 MeV (lower panel). The different colors in the figures represent the relative abundance of the particles considered as function of the baryonic density . ...
Context 2
... free case. Every drop of the hyperonic curves corresponds to an appearance of a new hyperon species into the star core. This is particularly visible at the lowest shown temperature of = 10, because the onset of hyperons is more abrupt. Note that, in the neutrino-free = 10 case, three hyperonic species appear at a very similar density (see Fig. 1) and this is visualized as a single drop in the corresponding thermal index curve. At higher temperatures the hyperons are already present at the lower densities in the core, so the thermal index has a smoother behaviour. We can also see that at higher lepton fractions ( = 0.4), as matter is more isospin symmetric, the chemical ...
Context 3
... this subsection we show the composition of the star for the abovementioned different cases. In Figure 1 the composition of a neutrino free neutron star core is shown for temperatures = 5 MeV (upper panel) and = 50 MeV (lower panel). The different colors in the figures represent the relative abundance of the particles considered as function of the baryonic density . ...
Context 4
... free case. Every drop of the hyperonic curves corresponds to an appearance of a new hyperon species into the star core. This is particularly visible at the lowest shown temperature of = 10, because the onset of hyperons is more abrupt. Note that, in the neutrino-free = 10 case, three hyperonic species appear at a very similar density (see Fig. 1) and this is visualized as a single drop in the corresponding thermal index curve. At higher temperatures the hyperons are already present at the lower densities in the core, so the thermal index has a smoother behaviour. We can also see that at higher lepton fractions ( = 0.4), as matter is more isospin symmetric, the chemical ...

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