2007/12/17 by Chihiro Sasaki, C. Sasaki, Bengt Friman +2 · 2 citations
Earth and Planetary Sciences · Physics and Astronomy · #Condensed matter physics #Critical exponent #Critical point (mathematics) #High-Energy Particle Collisions Research #High-pressure geophysics and materials #Observable #Phase (matter) #Phase diagram #Phase transition #Physics #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Scaling #Spinodal #Spinodal decomposition #Thermodynamics #Tricritical point #hep-ph #nucl-th
paper · pdf · doi:10.1103/physrevd.77.034024
published as Phys.Rev.D77:034024,2008 · 12 pages, 11 figures
arxiv created 2007/12/17 · openalex publication_date 2008/02/27 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The thermodynamics of a first-order chiral phase transition is considered in the presence of spinodal phase separation within the Nambu--Jona-Lasinio model. The properties of the basic thermodynamic observables in the coexistence phase are discussed for zero and nonzero quark masses. We focus on observables that probe the chiral phase transition. In particular, the behavior of the specific heat and entropy as well as charge fluctuations are calculated and analyzed. We show that the specific heat and charge susceptibilities diverge at the isothermal spinodal lines. We determine the scaling behavior and compute the critical exponent \ensuremathγ of the net quark number susceptibility at the isothermal spinodal lines within the Nambu--Jona-Lasinio model and the Ginsburg-Landau theory. We show that in the chiral limit the critical exponent \ensuremathγ=1/2 at the tricritical point as well as along the isothermal spinodal lines. On the other hand, for finite quark masses the critical exponent at the spinodal lines, \ensuremathγ=1/2, differs from that at the critical end point, \ensuremathγ=2/3, indicating a change in the universality class. These results are independent of the particular choice of the chiral Lagrangian and should be common for all mean-field approaches.