Scientists narrow the anchor point in a quantum chromodynamics critical point search

Scientists narrow the anchor point in a quantum chromodynamics critical point search
Left: tracks in the STAR detector from collisions of a 3.85 GeV gold beam in the Relativistic Heavy Ion Collider hitting a gold target from the left. Upper right: radial projection perpendicular to the beam. Lower right: side projection along the beam. Credit: STAR Collaboration

Heavy ion collisions at the highest energies have revealed a new phase of nuclear matter with freely moving quarks and gluons, the Quark Gluon Plasma (QGP). The Beam Energy Scan program at the RHIC particle accelerator, a Department of Energy (DOE) Office of Science user facility at Brookhaven National Laboratory, has enabled the study of the transition between QGP and hadronic matter over a wide energy range.

It revealed clear evidence that gold-gold collisions at the lowest energies accessible produce predominantly hadronic matter. In contrast, experiments at 20 GeV and above form a gluon plasma.

At collision energies of 3 GeV, the data taken by the STAR experiment in the fixed target mode can be reproduced by theoretical model calculations that only consider hadronic interactions. In addition, researchers have measured kinematic distributions for the first time for light hyper-nuclei that involve hadrons with strange quarks as well as ordinary nucleons (protons and neutrons). This is the beginning of the era for studying hyperon-nucleon interaction, an essential step for understanding the inner structure of compact stars.

Nuclear matter consists of interacting quarks and gluons, described by the theory of quantum chromodynamics (QCD). Like ordinary matter, it can exist in different phases, in today's world predominantly as protons and neutrons in atomic nuclei. Collisions of heavy nuclei provide a unique environment to study its properties.

The well-known hadronic phase of nuclear matter consists of baryons (protons and neutrons) and a large number of elementary particles. Heavy ion collisions have revealed a new phase of nuclear matter with freely moving quarks and gluons, the Quark Gluon Plasma (QGP). The QGP is like the matter in the and in dense compact stars. Despite these discoveries, the structure of nuclear matter and the transition between its hadronic and QGP phases are largely unknown.

Scientists are aiming to establish whether a critical point exists in the phase diagram of . At this critical point, the QGP would coexist with a gas of protons, neutrons, and other particles.

The scientists have recently found that gold-gold collisions at the lowest energies accessible at the Relativistic Heavy Ion Collider (RHIC) do not form a QGP, while at energies above 20 giga-electron volts (GeV) the QGP is observed. This indicates that the , if it exists, should be between energies of 3 GeV and 20 GeV. This research is an important step in mapping the structure and phases of quantum chromodynamics.

The related research has been published in Physics Letters B and Physical Review Letters.

More information: M.S. Abdallah et al, Disappearance of partonic collectivity in sNN=3GeV Au+Au collisions at RHIC, Physics Letters B (2022). DOI: 10.1016/j.physletb.2022.137003

M.S. Abdallah et al, Probing strangeness canonical ensemble with K−, ϕ(1020) and Ξ− production in Au+Au collisions at sNN=3 GeV, Physics Letters B (2022). DOI: 10.1016/j.physletb.2022.137152

M. S. Abdallah et al, Measurements of Proton High-Order Cumulants in sNN=3 GeV Au+Au Collisions and Implications for the QCD Critical Point, Physical Review Letters (2022). DOI: 10.1103/PhysRevLett.128.202303

M. S. Abdallah et al, Measurements of HΛ3 and HΛ4 Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region, Physical Review Letters (2022). DOI: 10.1103/PhysRevLett.128.202301

Citation: Scientists narrow the anchor point in a quantum chromodynamics critical point search (2022, December 6) retrieved 19 April 2024 from https://phys.org/news/2022-12-scientists-narrow-anchor-quantum-chromodynamics.html
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