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Related papers: Quark Gluon Plasma - Recent Advances

200 papers

At high temperatures, strongly interacting matter becomes a plasma of deconfined quarks and gluons. In statistical QCD, deconfinement and the properties of the resulting quark-gluon plasma can be investigated by studying the in-medium…

Nuclear Theory · Physics 2009-01-15 Binoy Krishna Patra , Vinod Chandra , Vineet Agotiya

$J/\psi$ measurements in $p+p$ and $d+Au$ collisions serve as crucial references to understand the $J/\psi$ production in $Au+Au$ collisions at RHIC where quark gluon plasma (QGP) is expected to be formed. They also provide important clues…

Nuclear Experiment · Physics 2016-09-08 W. Xie

This is a review of the Quantum Chromodynamics Cosmological Phase Transitions, the Quark-Gluon Plasma, the production of heavy quark states via p-p collisions and RHIC (Relativistic Heavy Ion Collisions) using the mixed hybrid theory for…

High Energy Physics - Phenomenology · Physics 2016-02-09 Leonard S. Kisslinger , Debasish Das

Quark coalescence predictions for various multi-strange baryon to anti-baryon ratios for central Au+Au collisions at RHIC energies are compared to preliminary data of the STAR collaboration. The formation of Quark Matter and the sudden…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Zimanyi , P. Levai , T. Csorgo , T. S. Biro

We calculate the direct photon yield in central and mid-peripheral Au+Au collisions at the Relativistic Heavy-Ion Collider (RHIC). The processes involving the propagation of jets have been convolved with a leading order treatment of jet…

High Energy Physics - Phenomenology · Physics 2009-11-11 Simon Turbide , Charles Gale

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

It has been theorized that if heavy nuclei (e.g. Au, Pb) are collided at sufficiently high energies, we might be to recreate the conditions that existed in the universe a few microseconds after the Big Bang. The kinetic energy of the…

Nuclear Experiment · Physics 2007-07-18 Anuj K. Purwar

For the past decade, measurements of semi-inclusive single identified particle spectra and two particle correlations in p-p and A+A collisions at RHIC have produced a treasure trove of results which indicate that the medium produced in…

Nuclear Experiment · Physics 2012-11-16 Michael J. Tannenbaum

The discovery and characterization of hot and dense QCD matter, known as Quark Gluon Plasma (QGP), remains the most international collaborative effort and synergy between theorists and experimentalists in modern nuclear physics to date. The…

The physics of heavy-ion collisions is one of the most exciting and challenging directions of science for the last four decades. On the theoretical side one deals with a non-abelian field theory, while on the experimental side today's…

Nuclear Theory · Physics 2025-04-22 Marcus Bleicher , Elena Bratkovskaya

The historical context of the recent results from high energy heavy ion reactions devoted to the search of quark-gluon plasma (QGP) is reviewed, with emphasis on the surprises encountered. The evidence for QGP from heavy ion reactions is…

High Energy Physics - Phenomenology · Physics 2009-11-11 Richard M. Weiner

These proceedings represent a brief overview of the exciting physics coming out from the Relativistic Heavy Ion Collider (RHIC) at Brookhaven National Laboratory. The experimental results from BRAHMS, PHOBOS, PHENIX and STAR indicate a…

Nuclear Experiment · Physics 2010-11-05 J. L. Nagle

The main goals of relativistic heavy-ion experiments is to study the properties of QCD matter under extreme temperatures and densities. The focus of this talk is the studies that are underway at the Relativistic Heavy Ion Collider (RHIC),…

Nuclear Experiment · Physics 2009-11-18 Helen Caines

The PHENIX collaboration presents a concept for a major upgrade to the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). This upgrade, referred to as sPHENIX, brings exciting new capability to the RHIC program by opening new…

Nuclear Experiment · Physics 2012-07-30 A. Adare , C. Aidala , N. N. Ajitanand , Y. Akiba , R. Akimoto , J. Alexander , K. Aoki , N. Apadula , H. Asano , E. T. Atomssa , T. C. Awes , B. Azmoun , V. Babintsev , M. Bai , X. Bai , N. Bandara , B. Bannier , K. N. Barish , O. Baron , B. Bassalleck , S. Bathe , V. Baublis , S. Baumgart , A. Bazilevsky , M. Beaumier , R. Belmont , G. Benjamin , A. Berdnikov , Y. Berdnikov , X. Bing , D. Black , J. Blackburn , D. S. Blau , M. Bobrek , J. Bok , S. Boose , K. Boyle , C. L. Britton , M. L. Brooks , J. Bryslawskyj , V. Bumazhnov , C. Butler , S. Butsyk , S. Campbell , A. Carollo , J. -S. Chai , C. -H. Chen , S. Chernichenko , C. Y. Chi , M. Chiu , I. J. Choi , J. B. Choi , S. Choi , S. Chollet , P. Christiansen , T. Chujo , V. Cianciolo , B. A. Cole , N. Cronin , N. Crossett , L. D'Orazio , S. Dairaku , A. Datta , M. S. Daugherity , G. David , K. DeBlasio , A. Debraine , K. Dehmelt , A. Denisov , A. Deshpande , E. J. Desmond , O. Dietzsch , L. Ding , A. Dion , J. H. Do , M. Donadelli , O. Drapier , A. Drees , K. A. Drees , J. M. Durham , A. Durum , L. Eberle , S. Edwards , Y. V. Efremenko , T. Engelmore , A. Enokizono , S. Esumi , K. O. Eyser , B. Fadem , D. E. Fields , M. Finger , M. Finger , F. Fleuret , S. L. Fokin , J. E. Frantz , A. Franz , A. D. Frawley , Y. Fukao , T. Fusayasu , K. Gainey , C. Gal , P. Garg , A. Garishvili , I. Garishvili , F. Gastaldi , H. Ge , P. Giannotti , F. Giordarno , A. Glenn , X. Gong , M. Gonin , Y. Goto , R. Granier de Cassagnac , N. Grau , S. V. Greene , M. Grosse Perdekamp , Y. Gu , T. Gunji , H. Guragain , J. S. Haggerty , K. I. Hahn , H. Hamagaki , S. Y. Han , J. Hanks , K. Hashimoto , R. Hayano , S. Hayashi , X. He , T. K. Hemmick , T. Hester , J. C. Hill , M. Hoefferkamp , R. S. Hollis , K. Homma , B. Hong , Y. Hori , T. Hoshino , J. Huang , S. Huang , J. R. Hutchins , T. Ichihara , Y. Ikeda , K. Imai , Y. Imazu , J. Imrek , M. Inaba , A. Iordanova , D. Isenhower , A. Isinhue , D. Ivanischev , V. Ivanov , B. V. Jacak , S. J. Jeon , M. Jezghani , J. Jia , X. Jiang , B. M. Johnson , K. S. Joo , D. Jouan , D. S. Jumper , J. Kamin , S. Kanda , B. H. Kang , J. H. Kang , J. S. Kang , J. Kapustinsky , K. Karatsu , D. Kawall , A. V. Kazantsev , H. -J. Kehayias , J. A. Key , V. Khachatryan , P. K. Khandai , A. Khanzadeev , K. M. Kijima , C. Kim , D. H. Kim , D. J. Kim , E. -J. Kim , H. J. Kim , K. -B. Kim , Y. -J. Kim , Y. K. Kim , E. Kistenev , J. Klatsky , D. Kleinjan , P. Kline , T. Koblesky , L. Kochenda , M. Kofarago , Y. Komatsu , B. Komkov , J. Koster , D. Kotchetkov , D. Kotov , P. Kravtsov , F. Krizek , K. Kurita , M. Kuriyama , M. Kurosawa , Y. Kwon , R. Lacey , Y. S. Lai , J. G. Lajoie , A. Lebedev , G. H. Lee , J. Lee , K. B. Lee , K. S. Lee , S. H. Lee , R. Lefferts , M. J. Leitch , M. A. L. Leite , M. Leitgab , B. Lewis , X. Li , S. H. Lim , A. Lipski , M. X. Liu , B. Love , D. Lynch , M. Lynch , C. F. Maguire , Y. I. Makdisi , M. Makek , A. Manion , V. I. Manko , E. Mannel , T. Maruyama , S. Masumoto , M. McCumber , P. L. McGaughey , D. McGlinchey , R. McKay , C. McKinney , A. Meles , M. Mendoza , R. Menegasso , B. Meredith , Y. Miake , T. Mibe , A. C. Mignerey , A. Milov , D. K. Mishra , J. T. Mitchell , S. Miyasaka , S. Mizuno , A. K. Mohanty , D. P. Morrison , M. Moskowitz , S. Motschwiller , T. V. Moukhanova , T. Murakami , J. Murata , A. Mwai , T. Nagae , S. Nagamiya , J. L. Nagle , M. I. Nagy , I. Nakagawa , Y. Nakamiya , K. R. Nakamura , T. Nakamura , K. Nakano , C. Nattrass , A. Nederlof , P. K. Netrakanti , M. Nihashi , T. Niida , K. Ninomiya , D. Northacker , R. Nouicer , T. Novak , N. Novitzky , A. Nukariya , A. S. Nyanin , E. O'Brien , C. A. Ogilvie , H. Oide , K. Okada , A. Oskarsson , K. Ozawa , R. Pak , C. Pancake , V. Pantuev , V. Papavassiliou , I. H. Park , S. Park , S. K. Park , S. F. Pate , L. Patel , J. -C. Peng , D. Perepelitsa , G. D. N. Perera , D. Yu. Peressounko , J. Perry , R. Petti , C. Pinkenburg , R. P. Pisani , J. Popule , M. L. Purschke , H. Qu , S. Radhakrishnan , J. Rak , I. Ravinovich , K. F. Read , R. Reynolds , V. Riabov , Y. Riabov , E. Richardson , N. Riveli , D. Roach , S. D. Rolnick , M. Rosati , E. Roschin , M. S. Ryu , A. Safonov , B. Sahlmueller , N. Saito , T. Sakaguchi , H. Sako , V. Samsonov , M. Sano , M. Sarsour , S. Sato , S. Sawada , B. Schaefer , K. Sedgwick , J. Seele , R. Seidl , Y. Sekiguchi , A. Sen , R. Seto , P. Sett , E. Shafto , D. Sharma , A. Shaver , I. Shein , T. -A. Shibata , K. Shigaki , M. Shimomura , K. Shoji , P. Shukla , P. Sicho , A. Sickles , C. L. Silva , D. Silvermyr , B. K. Singh , C. P. Singh , V. Singh , F. W. Sippach , M. Skolnik , S. Solano , A. Soldatov , R. A. Soltz , W. E. Sondheim , S. P. Sorensen , M. Soumya , I. V. Sourikova , P. K. Srivastava , P. W. Stankus , P. Steinberg , E. Stenlund , M. Stepanov , A. Ster , L. Stevens , S. P. Stoll , M. R. Stone , T. Sugitate , A. Sukhanov , J. Sun , J. Sziklai , E. M. Takagui , A. Takahara , A. Taketani , Y. Tanaka , K. Tanida , M. J. Tannenbaum , S. Tarafdar , A. Taranenko , A. Tate , E. Tennant , E. Thorsland , A. Timilsina , T. Todoroki , H. Torii , R. Towell , R. S. Towell , V. Trofimov , I. Tserruya , T. Tsuji , A. Tullo , H. W. van Hecke , M. Vargyas , E. Vazquez-Zambrano , A. Veicht , J. Velkovska , M. Virius , V. Vrba , E. Vznuzdaev , X. R. Wang , D. Watanabe , K. Watanabe , Y. Watanabe , Y. S. Watanabe , T. S. Watson , F. Wei , R. Wei , S. Whitaker , D. Winter , S. Wolin , C. L. Woody , M. Wysocki , Y. L. Yamaguchi , R. Yang , A. Yanovich , S. Yokkaichi , I. Yoon , M. Young , I. Younus , I. E. Yushmanov , W. A. Zajc , E. Zarndt , A. Zelenski , L. Zhang , S. Zhou , C. Zumberge

We investigate the onset of wave-breaking in the quark-gluon plasma (QGP) formed in heavy-ion collisions at both RHIC and the LHC. A nonlinear longitudinal color field is coupled to a three-dimensional viscous hydrodynamic background…

Nuclear Theory · Physics 2025-09-11 Biswarup Paul

Heavy quarks are good probes of the hot and dense medium created in relativistic heavy ion collisions since they are mainly generated early in the collision and interact with the medium in all collision stages. In addition, heavy flavor…

Nuclear Experiment · Physics 2019-08-13 Rachid Nouicer

The main goal of the experimental programs on ultra-relativistic heavy ion collisions at the LHC is the production and characterization of the Quark Gluon Plasma (QGP), a phase of nuclear matter in which strongly interacting constituents…

Nuclear Experiment · Physics 2016-08-08 Riccardo Russo

The first decade of RHIC running has established the existence of a strongly coupled Quark Gluon Plasma (sQGP), a new state of nuclear matter with partonic degrees of freedom. Theory predicts how transitions to this sQGP depend on the…

Nuclear Experiment · Physics 2019-08-13 Helen Caines

Ultrarelativistic heavy-ion collisions at the Relativistic Heavy Ion Collider (RHIC) are thought to have produced a state of matter called the quark-gluon plasma, characterized by a very small shear-viscosity to entropy-density ratio…

Nuclear Theory · Physics 2009-11-18 N. Demir , S. A. Bass