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Temperature measurement of Quark-Gluon plasma at different stages

  • STAR Collaboration
  • Texas A&M University
  • Goethe University Frankfurt
  • Brookhaven National Laboratory
  • Argonne National Laboratory
  • Tsinghua University
  • Central China Normal University
  • Fudan University
  • Lanzhou University
  • University of Illinois at Chicago
  • Shandong University
  • Guangxi Normal University
  • CAS - Institute of Modern Physics
  • University of Science and Technology of China
  • South China Normal University
  • Chongqing University
  • Warsaw University of Technology
  • Lawrence Berkeley National Laboratory
  • Academia Sinica Taiwan HQ
  • National Cheng Kung University
  • Stony Brook University
  • Kent State University
  • Huzhou University
  • Purdue University
  • University of Chinese Academy of Sciences
  • University of California at Los Angeles
  • United States Naval Academy
  • Indiana University Bloomington
  • Michigan State University
  • Heidelberg University 
  • AGH University of Krakow

Research output: Contribution to journalArticlepeer-review

7 Scopus citations

Abstract

In a Quark-Gluon Plasma (QGP), the fundamental building blocks of matter, quarks and gluons, are under extreme conditions of temperature and density. A QGP could exist in the early stages of the Universe, and in various objects and events in the cosmos. The thermodynamic and hydrodynamic properties of the QGP are described by Quantum Chromodynamics (QCD) and can be studied in heavy-ion collisions. Despite being a key thermodynamic parameter, the QGP temperature is still poorly known. Thermal lepton pairs (e+e and μ+μ) are ideal penetrating probes of the true temperature of the emitting source, since their invariant-mass spectra suffer neither from strong final-state interactions nor from blue-shift effects due to rapid expansion. Here we measure the QGP temperature using thermal e+e production at the Relativistic Heavy Ion Collider (RHIC). The average temperature from the low-mass region (in-medium ρ0 vector-meson dominant) is (2.01 ± 0.23) × 1012 K, consistent with the chemical freeze-out temperature from statistical models and the phase transition temperature from Lattice QCD. The average temperature from the intermediate mass region (above the ρ0 mass, QGP dominant) is significantly higher at (3.25 ± 0.60) × 1012 K. This work provides essential experimental thermodynamic measurements to map out the QCD phase diagram and understand the properties of matter under extreme conditions.

Original languageEnglish
Article number9098
JournalNature Communications
Volume16
Issue number1
DOIs
StatePublished - Dec 2025

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