Abstract

We make a theoretical and experimental summary of the state-of-the-art status of hot and dense QCD matter studies on selected topics. We review the Beam Energy Scan program for the QCD phase diagram and present the current status of the search for the QCD critical point, particle production in high baryon density region, hypernuclei production, and global polarization effects in nucleus-nucleus collisions. The available experimental data in the strangeness sector suggests that a grand canonical approach in the thermal model at high collision energy makes a transition to the canonical ensemble behavior at low energy. We further discuss future prospects of nuclear collisions to probe properties of baryon-rich matter. Creation of a quark-gluon plasma at high temperature and low baryon density has been called the “Little-Bang” and, analogously, a femtometer-scale explosion of baryon-rich matter at lower collision energy could be called the “femto-nova”, which could possibly sustain substantial vorticity and a magnetic field for non-head-on collisions.

Highlights

  • Nuclei are bound states of protons and neutrons via the strong interaction

  • We focus on two puzzling quantum chromodynamics (QCD) features for the nucleons which are composed of Nc valence quarks and have a mass, mN 940 MeV ∼ Nc QCD

  • This way of representating the results of experimental measurements and theory calculations serve to demonstrate clearly that the freeze-out density and K+/π + ratio could be related. (d) The K−/π − ratio seems unaffected by the changes in the Through these measurements we have the knowledge of regions in collision energy where the maximal net-baryon density is reached

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Summary

Introduction

Nuclei are bound states of protons and neutrons via the strong interaction. The fundamental theory of the strong interaction is quantum chromodynamics (QCD). The idea of using the relativistic nucleus-nucleus collisions or heavy-ion collisions is to shake the QCD vacuum with high energy density to observe new states of matter out of quarks and gluons and to seek for traces of phase transitions associated with confinement and/or chiral symmetry breaking By adjusting the collision energy in the heavy-ion collisions, the baryon density could transiently increase up to several times of ρ0 according to numerical simulations [7]. Such a femtometer-scale explosion of baryon rich matter can be called the femtonova. We will first describe the phase diagram, the QCD critical point, and properties of baryon-rich matter including strangeness degrees of freedom. We discuss the future directions of ongoing experimental projects as well as future experimental facilities

Theoretical background for the QCD phase diagram
Observables for the QCD critical point
Baryon-rich matter, an approximate triple point, and strangeness
QCD critical point search
High baryon density matter
Lifetime of hypernuclei
Polarization and spin alignment
QCD phase structures and quark matter at high baryon density
Neutron star phenomenology
Femto-nova rotating with magnetic fields
More on the QCD critical point
Light hypernuclei production
Fluid vorticity of high baryon density matter
Future experimental facilities for high baryon density matter
NICA a JINR
CBM a FAIR
JPARC-HI a KEK/JAEA
Conclusions
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