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Related papers: Phase diagram determination at fivefold nuclear co…

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We discuss an outside-inside scenario for a first order quark-hadron transition in the Quark-Gluon Plasma (QGP) expected to be produced in heavy ion collisions, wherein the entire QGP region itself becomes like a subcritical bubble, and…

High Energy Physics - Phenomenology · Physics 2009-10-30 Sanatan Digal , Ajit M. Srivastava

We analyze fluctuations of quark number and electric charge, in 2-flavour QCD at finite temperature and vanishing net baryon number density. In the hadronic phase we find that an enhancement of charge fluctuations arises from contributions…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. Karsch , S. Ejiri , K. Redlich

Recent indications for high neutron star masses (M \sim 2 M_sun) and large radii (R > 12 km) could rule out soft equations of state and have provoked a debate whether the occurence of quark matter in compact stars can be excluded as well.…

Nuclear Theory · Physics 2017-08-23 D. B. Blaschke , T. Klahn , F. Sandin

We analyze multiparticle production in a thermal framework for 7 central nucleus nucleus collisions, $e^+$+ $e^-$ annihilation into hadrons on the Z resonance and 4 hadronic reactions (p+p and p+$\bar{p}$ with partial centrality selec…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sonja Kabana , Peter Minkowski

The Parton-Hadron-String Dynamics (PHSD) transport approach consistently simulates the full evolution of a relativistic heavy-ion collision from the initial hard scatterings string formation through the dynamical deconfinement phase…

Nuclear Theory · Physics 2014-11-20 O. Linnyk , E. L. Bratkovskaya , W. Cassing

Recent observations of neutron stars, combined with causality, thermodynamic stability, and nuclear constraints, indicate a rapid stiffening of QCD matter at densities slightly above nuclear saturation density ($n_0 \simeq 0.16\,{\rm…

Nuclear Theory · Physics 2025-06-16 Toru Kojo

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 analyse the nucleation of quark matter droplets under protoneutron star conditions. We adopt a two-phase framework in which the hadronic phase is described through a non-linear Walecka model and the just deconfined matter by the MIT bag…

High Energy Physics - Phenomenology · Physics 2013-08-21 T. A. S. do Carmo , G. Lugones , A. G. Grunfeld

This is an introduction to the use of nonperturbative flow equations in strong interaction physics at nonzero temperature and baryon density. We investigate the QCD phase diagram as a function of temperature, chemical potential for baryon…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Berges

Thermodynamical properties of the nuclear matter at sub-saturation densities were investigated using a simple van der Waals-like equation of state with an additional term representing the symmetry energy. First-order isospin-asymmetric…

Nuclear Theory · Physics 2009-11-13 M. Veselsky

We present a review of the studies related to establishing the QCD phase diagram through high energy nucleus-nucleus collisions. We particularly focus on the experimental results related to the formation of a quark-gluon phase, crossover…

Nuclear Experiment · Physics 2015-06-17 Bedangadas Mohanty

We study the cooling behaviour of an isolated strange quark star, using an equation of state derived from perturbative QCD up to second order in strong coupling constant, and we compare it with that of a neutron star. After an initial rapid…

Astrophysics · Physics 2007-05-23 K. -W. Wong , M. -C. Chu

Ultrarelativistic heavy ion collisions recreate in the laboratory the thermodynamical conditions prevailing in the early universe up to 10$^{-6}$ seconds, thereby allowing the study of the quark-gluon plasma (QGP), a state of quantum…

High Energy Physics - Experiment · Physics 2020-11-26 CMS Collaboration

We describe the properties of quark matter at zero temperature and finite baryon densities within microscopic Vlasov/molecular dynamics approaches. We use an inter-quark Richardson's potential consistent with the indications of Lattice QCD…

Nuclear Theory · Physics 2016-09-08 A. Bonasera

The theory of confinement and deconfinement is discussed as based on the properties of the QCD vacuum. The latter are described by field correlators of colour-electric and colour-magnetic fields in the vacuum, which can be calculated…

High Energy Physics - Phenomenology · Physics 2015-05-13 A. V. Nefediev , Yu. A. Simonov , M. A. Trusov

The recent detection of gravitational waves from merging neutron star events has opened a new window on the many unknown aspects of their internal dynamics. A key role in this context is played by the transition from baryon to quark matter…

High Energy Physics - Phenomenology · Physics 2019-10-08 Abha Rajan , Tyler Gorda , Simonetta Liuti , Kent Yagi

We study the confinement/deconfinement transition of QCD matter for a quark-gluon plasma at finite density using AdS/QCD duality. In order to determine the critical temperature and its dependence on the quark chemical potential, the…

High Energy Physics - Theory · Physics 2024-07-01 Nelson R. F. Braga , Octavio C. Junqueira

The chromo-magnetic monopoles (CMM), emergent topological excitations of non-Abelian gauge fields carrying chromo-magnetic charge, have long been postulated to play an important role in the vacuum confinement of quantum chromodynamics…

High Energy Physics - Phenomenology · Physics 2025-10-21 Yu Guo , Jinfeng Liao , Shuzhe Shi

The heavy quark collisional scattering on partons of the quark gluon plasma (QGP) is studied in a QCD medium at finite temperature and chemical potential. We evaluate the effects of finite parton masses and widths, finite temperature $T$…

High Energy Physics - Phenomenology · Physics 2015-05-11 H. Berrehrah , E. Bratkovskaya , W. Cassing , P. B. Gossiaux , J. Aichelin

High-energy nuclear collisions encompass three key stages: the structure of the colliding nuclei informed by low-energy nuclear physics, the initial condition (IC) leading to the formation of quark-gluon plasma (QGP), and the hydrodynamic…

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