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This lecture concerns the properties of strongly interacting matter (which is described by Quantum Chromodynamics) at very high energy density. I review the properties of matter at high temperature, discussing the deconfinement phase…

High Energy Physics - Phenomenology · Physics 2011-01-04 Larry McLerran

Heavy-ion collisions provide the only laboratory tests of relativistic quantum field theory at finite temperature. Understanding these is a necessary step in understanding the origins of our universe. These lectures introduce the subject to…

Nuclear Theory · Physics 2018-02-21 Sourendu Gupta

Despite that quantum chromodynamics, the theory of strong interaction, has colorful quarks and gluons as its basic degrees of freedom, all fundamental particles participating the strong interaction that can be directly detected in…

High Energy Physics - Phenomenology · Physics 2022-03-17 Feng-Kun Guo , Haiping Peng , Ju-Jun Xie , Xiaorong Zhou

The application of Riemannian geometry to the analysis of the equilibrium thermodynamics in Quantum Chromodynamics (QCD) at finite temperature and baryon density gives a new method to evaluate the critical temperature, $T_c$, of the…

Nuclear Theory · Physics 2020-12-16 Paolo Castorina , Mauro Imbrosciano , Daniele Lanteri

The vacuum is now understood to possess a rich and complex structure, characterized by fluctuating energy fields and a condensate of virtual quark-antiquark pairs. The spontaneous breaking of the approximate chiral symmetry, signaled by the…

High Energy Physics - Experiment · Physics 2026-02-10 The STAR Collaboration

In this conference proceeding, I discuss in detail the deconfinement to quark matter that takes place at large densities and/or temperatures. The first-order phase transition that is assumed to appear beyond a critical point gives rise to…

Nuclear Theory · Physics 2018-01-26 Veronica Dexheimer

After the discovery of the Quantum Chromodynamics (QCD), many experimental and theoretical efforts have been made to investigate physics issues involved in ultra relativistic heavy-ion collisions. The fundamental goal of this work is to…

High Energy Physics - Phenomenology · Physics 2012-08-28 Vlasios Petousis

Quantum Chromodynamics and Quantum Electrodynamics, both renormalizable quantum field theories with a small number of precisely constrained input parameters, dominate the dynamics of the quarks and gluons - the underlying building blocks of…

Nuclear Theory · Physics 2015-10-08 Martin J. Savage

In the last few years, numerical simulations of QCD on the lattice have reached a new level of accuracy. A wide range of thermodynamic quantities is now available in the continuum limit and for physical quark masses. This allows a…

High Energy Physics - Lattice · Physics 2018-07-25 Claudia Ratti

The strong interaction - governed by Quantum Chromodynamics (QCD) - shapes the structure of the visible universe. At about 10 $\mu$s after the big bang, the primordial matter made up of quarks and gluons plus leptons, photons and neutrinos,…

Nuclear Experiment · Physics 2026-01-27 Peter Braun-Munzinger , Anar Rustamov , Nu Xu

Mapping the QCD phase boundary and locating critical end point still remains as an open problem in strong interaction physics. Predictions about the co-ordinates of the critical point in the $(T, \mu_B)$ plane, from different QCD motivated…

High Energy Physics - Phenomenology · Physics 2011-01-26 Partha Pratim Bhaduri , Victor Roy , A. K. Chaudhuri

Quantum Chromodynamics (QCD) is a basic gauge field theory to describe strong interactions. Lattice QCD calculations predict a phase transition from hadronic matter to a deconfined, locally thermalized Quark-Gluon Plasma (QGP) state at high…

Nuclear Experiment · Physics 2007-05-23 Xin Dong

We study analytically the phase diagram of the pure $SU(N)$ lattice gauge theory at finite temperature, and we attempt to estimate the critical deconfinement temperature. We apply large $N$ techniques to the Wilson and to the Heat Kernel…

High Energy Physics - Lattice · Physics 2009-10-22 M. Billo' , M. Caselle , A. D'Adda , L. Magnea , S. Panzeri

We clarify the conditions of the cosmic quantum chromodynamics (QCD) first-order phase transition in the early universe by carefully distinguishing the chiral and deconfinement phase transitions. While the chiral one with light quarks at…

High Energy Physics - Phenomenology · Physics 2024-05-02 Fei Gao , Sichun Sun , Graham White

Quantum chromodynamics (QCD) reduces the strong interactions, in all their variety, to a simple nonabelian gauge theory. It clearly and elegantly explains hadrons at short distances, which has led to its universal acceptance. Since its…

High Energy Physics - Lattice · Physics 2012-11-13 Andreas S. Kronfeld

At sufficiently high temperature and density, quantum chromodynamics (QCD) is expected to undergo a phase transition from the confined phase to the quark-gluon plasma phase. In the Lagrangian lattice formulation the Monte Carlo method works…

High Energy Physics - Lattice · Physics 2009-10-31 E. B. Gregory , S. Guo , H. Kroger , Xiang-Qian Luo

Thermodynamics of a heavy quark-antiquark pair in SU(3)-QCD is studied below the deconfinement critical temperature, $T_c$. In the quenched case, a model of the string passing through heavy valence gluons yields a correct estimate of $T_c$…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Antonov , S. Domdey , H. -J. Pirner

Hot QCD physics studies the nuclear strong force under extreme temperature and densities. Experimentally these conditions are achieved via high-energy collisions of heavy ions at the Relativistic Heavy Ion Collider (RHIC) and the Large…

Nuclear Experiment · Physics 2023-03-31 M. Arslandok , S. A. Bass , A. A. Baty , I. Bautista , C. Beattie , F. Becattini , R. Bellwied , Y. Berdnikov , A. Berdnikov , J. Bielcik , J. T. Blair , F. Bock , B. Boimska , H. Bossi , H. Caines , Y. Chen , Y. -T. Chien , M. Chiu , M. E. Connors , M. Csanád , C. L. da Silva , A. P. Dash , G. David , K. Dehmelt , V. Dexheimer , X. Dong , A. Drees , L. Du , J. M. Durham , R. J. Ehlers , H. Elfner , O. Evdokimov , M. Finger , M. Finger , J. Frantz , A. D. Frawley , C. Gale , F. Geurts , V. Gonzalez , N. Grau , S. V. Greene , S. K. Grossberndt , T. Hachiya , X. He , U. Heinz , B. Hong , T. J. Humanic , D. Ivanishchev , B. V. Jacak , J. Jahan , S. Jeon , H. R. Jheng , J. Jia , E. G. Judd , J. I. Kapusta , I. Karpenko , V. Khachatryan , D. E. Kharzeev , M. Kim , B. Kimelman , J. L. Klay , S. R. Klein , A. G. Knospe , V. Koch , D Kotov , G. K. Krintiras , R. Kunnawalkam Elayavalli , C. M. Kuo , J. G. Lajoie , Y. -J. Lee , W. Li , J. Liao , I. Likmeta , S. H. Lim , M. X. Liu , C. Loizides , R. Longo , X. Luo , M. Luzum , R. Ma , A. Majumder , S. Mak , C. Markert , Y. Mehtar-Tani , A. C. Mignerey , N. Minafra , D. P. Morrison , B. Mueller , J. L. Nagle , A. Narde , C. E. Nattrass , T. Niida , J. Noronha , J. Noronha-Hostler , R. Nouicer , N. Novitzky , E. O'Brien , G. Odyniec , V. A. Okorokov , J. D. Osborn , J. -F. Paquet , S. Park , P. Parotto , D. V. Perepelitsa , P. Petreczky , C. Pinkenburg , M. Praszalowicz , C. Pruneau , J. Putschke , N. V. Ramasubramanian , R. Rapp , C. Ratti , K. F. Read , P. Rebello Teles , R. Reed , T. Rinn , G. Roland , M. Rosati , C. Royon , L. Ruan , T. Sakaguchi , S. Salur , M. Sarsour , A. S. Menon , B. Schenke , N. V. Schmidt , A. Schmier , T. Schäfer , J. Seger , R. Seto , Oveis Sheibani , C. Shen , Z. Shi , E. Shulga , A. M. Sickles , M. Singh , B. K. Singh , N. Smirnov , K. L. Smith , H. Song , I. Soudi , A. G. Stahl Leiton , P. Steinberg , M. Stephanov , M. Strickland , M. Sumbera , D. Sunar Cerci , Y. Tachibana , A. H. Tang , D. Tapia Takaki , D. Teaney , D. Thomas , A. R. Timmins , P. Tribedy , Z. Tu , S. Tuo , O. V. Rueda , J. Velkovska , R. Venugopalan , F. Videbæk , S. A. Voloshin , V. Vovchenko , G. Vujanovic , X. Wang , F. Wang , X. -N. Wang , S. Weyhmiller , W. Xie , N. Xu , Y. Yang , X. Yao , Z. Ye , H. -U. Yee , W. A. Zajc

We discuss recent progress made studies of bulk thermodynamics of strongly interacting matter through lattice simulations of QCD with an almost physical light and strange quark mass spectrum. We present results on the QCD equation of state…

High Energy Physics - Lattice · Physics 2008-11-26 Frithjof Karsch

We present experimental features of identified particle production from nucleus-nucleus collisions at RHIC. These features reflect hadronization from a deconfined partonic matter whose particle formation scheme is distinctly different from…

Nuclear Experiment · Physics 2007-05-23 Huan Z. Huang