Spinodal instabilities of baryon-rich quark-gluon plasma in the Polyakov–Nambu–Jona-Lasinio model Academic Article uri icon

abstract

  • © 2016 American Physical Society. Using the Polyakov-Nambu-Jona-Lasinio model, we study the spinodal instability of a baryon-rich quark-gluon plasma in the linear response theory. We find that the spinodal unstable region in the temperature and density plane shrinks with increasing wave number of the unstable mode and is also reduced if the effect of the Polyakov loop is not included. In the small wave number or long wavelength limit, the spinodal boundaries in both cases of with and without the Polyakov loop coincide with those determined from the isothermal spinodal instability in the thermodynamic approach. Also, the vector interactions among quarks are found to suppress unstable modes of all wave numbers. Moreover, the growth rate of unstable modes initially increases with the wave number but is reduced when the wave number becomes large. Including the collisional effect from quark scattering via the linearized Boltzmann equation, we further find that it decreases the growth rate of unstable modes of all wave numbers. The relevance of these results to relativistic heavy ion collisions is discussed.

altmetric score

  • 0.75

author list (cited authors)

  • Li, F., & Ko, C. M.

citation count

  • 12

publication date

  • March 2016