2025/02/14 by Jens O. Andersen, Andersen, Jens O., Mathias P. Nødtvedt +1 · 2 citations
Physics and Astronomy · #Cold Atom Physics and Bose-Einstein Condensates #FOS: Physical sciences #High Energy Physics - Lattice (hep-lat) #High Energy Physics - Phenomenology (hep-ph) #High-Energy Particle Collisions Research #Nuclear Theory (nucl-th) #Quantum Chromodynamics and Particle Interactions
paper · pdf · doi:10.48550/arxiv.2502.10229
openalex publication_date 2025/02/14 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
We employ the two-flavor quark-meson diquark model as a low-energy model for QCD at non-zero quark and isospin chemical potentials μ and μI, and at zero temperature. We map out the phase diagram in the μ-μI plane, which has four phases: a vacuum phase, a phase with condensed charged pions/Cooper pairs of u and d quarks, a normal quark matter phase, and a color superconducting phase (2SC phase). %In the 2SC phase, we study the effects of imposing color and %electric charge neutrality. The global symmetry breaking SU(3)c→ SU(2)c in the 2SC phase gives rise to a number of Nambu-Goldstone bosons. We classify them and briefly discuss their properties. We calculate the speed of sound cs in the two special cases, finite μI and μ=0, and finite μ and μI=0. In both cases, the speed of sound exhibits a maximum and approaches the conformal limit from above as the density increases. For non-zero isospin μI, this behavior is in agreement with the speed of sound obtained from lattice simulations. In the 2SC phase, the behavior is qualitatively the same if we impose local charge neutrality. Finally, we discuss the possibility of having a mixed phase of negatively charged normal quark matter and positively charged 2SC matter with global color charge neutrality imposed on the latter.