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Related papers: Recent progress in hard-thermal-loop QCD thermodyn…

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Classical transport theory is employed to analyze the hot quark-gluon plasma at the leading order in the coupling constant. A condition on the (covariantly conserved) color current is obtained. {}From this condition, the generating…

High Energy Physics - Phenomenology · Physics 2011-05-05 P. F. Kelly , Q. Liu , C. Lucchesi , C. Manuel

In this review article, we discuss the current status and future prospects of perturbation theory as a means of studying the equilibrium thermodynamic and near-equilibrium transport properties of deconfined QCD matter. We begin with a brief…

High Energy Physics - Phenomenology · Physics 2020-10-14 Jacopo Ghiglieri , Aleksi Kurkela , Michael Strickland , Aleksi Vuorinen

Recent works have associated systems of particles, characterized by short-range repulsive interactions and evolving under overdamped motion, to a nonlinear Fokker-Planck equation within the class of nonextensive statistical mechanics, with…

Statistical Mechanics · Physics 2017-11-22 Andre M. C. Souza , Roberto F. S. Andrade , Fernando D. Nobre , Evaldo M. F. Curado

I review recent lattice results on strongly interacting matter under extreme conditions, with emphasis on the finite-temperature QCD transition at $\mu_B=0$, its approach toward the chiral limit and the fate of the $U_A(1)$ anomaly, as well…

High Energy Physics - Lattice · Physics 2026-05-12 Heng-Tong Ding

I review recent progress in study of strongly interacting matter at high temperatures using Monte-Carlo simulations in lattice QCD.

High Energy Physics - Lattice · Physics 2015-06-04 P. Petreczky

A study of QCD at non-zero chemical potential, mu, and temperature, T, is performed using the lattice technique. The transition temperature (between the confined and deconfined phases) is determined as a function of mu and is found to be in…

High Energy Physics - Phenomenology · Physics 2017-08-23 C. R. Allton , S. Ejiri , S. J. Hands , O. Kaczmarek , F. Karsch , E. Laermann , Ch. Schmidt , L. Scorzato

An effective field theory approach is developed for calculating the thermodynamic properties of a field theory at high temperature $T$ and weak coupling $g$. The effective theory is the 3-dimensional field theory obtained by dimensional…

High Energy Physics - Phenomenology · Physics 2016-09-01 Eric Braaten , Agustin Nieto

We compute the free energy density for gauge theories, with fermions, at high temperature and zero chemical potential. Specifically, we analytically compute the free energy through $O(g^4)$, which requires the evaluation of three-loop…

High Energy Physics - Phenomenology · Physics 2016-09-01 Peter Arnold , Chengxing Zhai

I review recent theoretical progress on the description of heavy quark, jet and gauge boson production at colliders within perturbative QCD. Particular emphasis is put on the improved understanding of fragmentation phenomena, resummation of…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Gehrmann

In high energy nucleus-nucleus collisions, a transient state of thermalized, hot and dense matter governed by Quantum Chromodynamics is produced. Properties of this state are reflected in the bulk low transverse momentum (P_T) hadron…

High Energy Physics - Phenomenology · Physics 2010-01-15 Thorsten Renk

We discuss the hard dense loop perturbation theory approach for studying the thermodynamics of strongly magnetized dense quark matter. The free energy of quarks and gluons have been calculated for one-loop quark and gluon self-energies,…

Nuclear Theory · Physics 2025-07-01 Sarthak Satapathy , Sumit , Salman Ahamad Khan

Two recent attempts for overcoming the poor convergence of the perturbation expansion of the thermodynamic potentials of QCD are discussed: an HTL-adaption of ``screened perturbation theory'' and approximately self-consistent HTL…

High Energy Physics - Phenomenology · Physics 2017-08-23 A. Rebhan

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 describe how thermalization occurs in heavy ion collisions in the framework of perturbative QCD. When the saturation scale $Q_s$ is large compared to $\Lambda_{QCD}$, thermalization takes place during a time of order…

High Energy Physics - Phenomenology · Physics 2011-05-05 R. Baier , A. H. Mueller , D. Schiff , D. T. Son

There has been significant progress in our understanding of finite-temperature field theory over the past decade. In this paper, we review the progress in perturbative thermal field theory focusing on thermodynamic quantities. We first…

High Energy Physics - Phenomenology · Physics 2009-09-29 Jens O. Andersen , M. Strickland

We use next-to-leading-order in perturbation theory to investigate the effects of a finite isospin density on the thermodynamics of cold strongly interacting matter. Our results include nonzero quark masses and are compared to lattice data.

High Energy Physics - Phenomenology · Physics 2016-08-03 Thorben Graf , Juergen Schaffner-Bielich , Eduardo S. Fraga

Quantum Molecular Dynamics (QMD) calculations of central collisions between heavy nuclei are used to study fragment production and the creation of collective flow. It is shown that the final phase space distributions are compatible with the…

It has been known for some time that the entropy of hot QCD is well reproduced by weak coupling techniques. These do not identify with perturbation theory, known to have poor convergence properties, but involve resumming the physics of hard…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jean-Paul Blaizot , Andreas Ipp , Anton Rebhan , Urko Reinosa

Recent results of lattice QCD at finite temperature and density are reviewed. At vanishing density the transition temperature, the equation of state and hadron properties are discussed both for the pure gauge theory and for dynamical…

High Energy Physics - Lattice · Physics 2009-11-10 S. D. Katz

Using generic properties of string theories, we show how interesting non-perturbative features of QCD can be exploited in heavy ion collisions. In particular, a generalized "semi-circle" law for the phase diagram in the temperature-chemical…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. C. Brower , J. McGreevy , C-I Tan
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