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The correlation between baryon number and strangeness elucidates the nature of strongly interacting matter, such as that formed transiently in high-energy nuclear collisions. This diagnostic can be extracted theoretically from lattice QCD…

Nuclear Theory · Physics 2009-02-05 V. Koch , A. Majumder , J. Randrup

In statistical QCD, the thermal properties of the quark-gluon plasma can be determined by studying the in-medium behaviour of heavy quark bound states. The results can be applied to quarkonium production in high energy nuclear collisions,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Helmut Satz

We investigate production of \phi mesons and \Xi baryons in nucleus-nucleus collisions. Reactions on strange particles acting as a catalyser are proposed to interpret the high observed \phi yields in HADES experiments as well as the energy…

Nuclear Theory · Physics 2015-03-19 Boris Tomasik , Evgeni E. Kolomeitsev

We show that the remaining internal longitudinal flow of colliding quarks in nuclei offers a natural explanation for the diversity of rapidity spectral shapes observed in Pb--Pb 158AGeV nuclear collisions. Thus QGP sudden hadronization…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jean Letessier , Johann Rafelski

We discuss recent experimental results in the field of ultra-relativistic nuclear collisions. The emerging ``picture'' is a collectively expanding, initially hot and dense fireball in which strangeness- and low-mass di-lepton pair…

Nuclear Experiment · Physics 2009-10-31 Peter Braun-Munzinger

We study multistrange hadrons produced in NA49 and STAR experiments at center of mass energies varying from \sqrt{s_{NN}} = 7.61 GeV to 200 GeV. We show that the yields of {\Xi}, {\Xi}-bar and {\phi} can help to constrain the physical…

High Energy Physics - Phenomenology · Physics 2011-03-02 Michal Petran , Jean Letessier , Vojtech Petracek , Jan Rafelski

A new channel of direct photon production from a quark gluon plasma (QGP) is explored in the framework of high-temperature QCD. This process appears at next-to-leading order, in the presence of a charge asymmetry in the excited matter. The…

High Energy Physics - Phenomenology · Physics 2010-11-26 Guang-You Qin , Abhijit Majumder , Charles Gale

The production of mesons containing strange quarks (K$^0_s$, $\phi$) and both singly and doubly strange baryons ($\Lambda$, Anti-$\Lambda$, and $\Xi$+Anti-$\Xi$) are measured at central rapidity in pp collisions at $\sqrt{s}$ = 0.9 TeV with…

High Energy Physics - Experiment · Physics 2017-09-29 ALICE Collaboration

We revisit the problem of the production of light atomic nuclei in ultrarelativistic heavy-ion collisions. While their production systematics is well produced by hadro-chemical freezeout at temperatures near the QCD pseudo-critical…

Nuclear Theory · Physics 2019-06-05 Xinyuan Xu , Ralf Rapp

We report the measurements of $\Sigma (1385)$ and $\Lambda (1520)$ production in $p+p$ and $Au+Au$ collisions at $\sqrt{s_{NN}} = 200$ GeV from the STAR collaboration. The yields and the $p_{T}$ spectra are presented and discussed in terms…

Nuclear Experiment · Physics 2010-07-27 The STAR collaboration , B. I. Abelev , M. M. Aggarwal , Z. Ahammed , J. Amonett , B. D. Anderson , M. Anderson , D. Arkhipkin , G. S. Averichev , Y. Bai , J. Balewski , O. Barannikova , L. S. Barnby , J. Baudot , S. Bekele , V. V. Belaga , A. Bellingeri-Laurikainen , R. Bellwied , F. Benedosso , S. Bhardwaj , A. Bhasin , A. K. Bhati , H. Bichsel , J. Bielcik , J. Bielcikova , L. C. Bland , S-L. Blyth , B. E. Bonner , M. Botje , J. Bouchet , A. V. Brandin , A. Bravar , T. P. Burton , M. Bystersky , R. V. Cadman , X. Z. Cai , H. Caines , M. Calderón de la Barca Sánchez , J. Castillo , O. Catu , D. Cebra , Z. Chajecki , P. Chaloupka , S. Chattopadhyay , H. F. Chen , J. H. Chen , J. Cheng , M. Cherney , A. Chikanian , W. Christie , J. P. Coffin , T. M. Cormier , M. R. Cosentino , J. G. Cramer , H. J. Crawford , D. Das , S. Das , S. Dash , M. Daugherity , M. M. de Moura , T. G. Dedovich , M. DePhillips , A. A. Derevschikov , L. Didenko , T. Dietel , P. Djawotho , S. M. Dogra , W. J. Dong , X. Dong , J. E. Draper , F. Du , V. B. Dunin , J. C. Dunlop , M. R. Dutta Mazumdar , V. Eckardt , W. R. Edwards , L. G. Efimov , V. Emelianov , J. Engelage , G. Eppley , B. Erazmus , M. Estienne , P. Fachini , R. Fatemi , J. Fedorisin , K. Filimonov , P. Filip , E. Finch , V. Fine , Y. Fisyak , J. Fu , C. A. Gagliardi , L. Gaillard , M. S. Ganti , L. Gaudichet , V. Ghazikhanian , P. Ghosh , J. E. Gonzalez , Y. G. Gorbunov , H. Gos , O. Grebenyuk , D. Grosnick , S. M. Guertin , K. S. F. F. Guimaraes , N. Gupta , T. D. Gutierrez , B. Haag , T. J. Hallman , A. Hamed , J. W. Harris , W. He , M. Heinz , T. W. Henry , S. Hepplemann , B. Hippolyte , A. Hirsch , E. Hjort , A. M. Hoffman , G. W. Hoffmann , M. J. Horner , H. Z. Huang , S. L. Huang , E. W. Hughes , T. J. Humanic , G. Igo , P. Jacobs , W. W. Jacobs , P. Jakl , F. Jia , H. Jiang , P. G. Jones , E. G. Judd , S. Kabana , K. Kang , J. Kapitan , M. Kaplan , D. Keane , A. Kechechyan , V. Yu. Khodyrev , B. C. Kim , J. Kiryluk , A. Kisiel , E. M. Kislov , S. R. Klein , A. Kocoloski , D. D. Koetke , T. Kollegger , M. Kopytine , L. Kotchenda , V. Kouchpil , K. L. Kowalik , M. Kramer , P. Kravtsov , V. I. Kravtsov , K. Krueger , C. Kuhn , A. I. Kulikov , A. Kumar , A. A. Kuznetsov , M. A. C. Lamont , J. M. Landgraf , S. Lange , S. LaPointe , F. Laue , J. Lauret , A. Lebedev , R. Lednicky , C-H. Lee , S. Lehocka , M. J. LeVine , C. Li , Q. Li , Y. Li , G. Lin , X. Lin , S. J. Lindenbaum , M. A. Lisa , F. Liu , H. Liu , J. Liu , L. Liu , Z. Liu , T. Ljubicic , W. J. Llope , H. Long , R. S. Longacre , W. A. Love , Y. Lu , T. Ludlam , D. Lynn , G. L. Ma , J. G. Ma , Y. G. Ma , D. Magestro , D. P. Mahapatra , R. Majka , L. K. Mangotra , R. Manweiler , S. Margetis , C. Markert , L. Martin , H. S. Matis , Yu. A. Matulenko , C. J. McClain , T. S. McShane , Yu. Melnick , A. Meschanin , J. Millane , M. L. Miller , N. G. Minaev , S. Mioduszewski , C. Mironov , A. Mischke , D. K. Mishra , J. Mitchell , B. Mohanty , L. Molnar , C. F. Moore , D. A. Morozov , M. G. Munhoz , B. K. Nandi , C. Nattrass , T. K. Nayak , J. M. Nelson , P. K. Netrakanti , L. V. Nogach , S. B. Nurushev , G. Odyniec , A. Ogawa , V. Okorokov , M. Oldenburg , D. Olson , M. Pachr , S. K. Pal , Y. Panebratsev , S. Y. Panitkin , A. I. Pavlinov , T. Pawlak , T. Peitzmann , V. Perevoztchikov , C. Perkins , W. Peryt , S. C. Phatak , R. Picha , M. Planinic , J. Pluta , N. Poljak , N. Porile , J. Porter , A. M. Poskanzer , M. Potekhin , E. Potrebenikova , B. V. K. S. Potukuchi , D. Prindle , C. Pruneau , J. Putschke , G. Rakness , R. Raniwala , S. Raniwala , R. L. Ray , S. V. Razin , J. Reinnarth , D. Relyea , F. Retiere , A. Ridiger , H. G. Ritter , J. B. Roberts , O. V. Rogachevskiy , J. L. Romero , A. Rose , C. Roy , L. Ruan , M. J. Russcher , R. Sahoo , T. Sakuma , S. Salur , J. Sandweiss , M. Sarsour , P. S. Sazhin , J. Schambach , R. P. Scharenberg , N. Schmitz , K. Schweda , J. Seger , I. Selyuzhenkov , P. Seyboth , A. Shabetai , E. Shahaliev , M. Shao , M. Sharma , W. Q. Shen , S. S. Shimanskiy , E Sichtermann , F. Simon , R. N. Singaraju , N. Smirnov , R. Snellings , G. Sood , P. Sorensen , J. Sowinski , J. Speltz , H. M. Spinka , B. Srivastava , A. Stadnik , T. D. S. Stanislaus , R. Stock , A. Stolpovsky , M. Strikhanov , B. Stringfellow , A. A. P. Suaide , E. Sugarbaker , M. Sumbera , Z. Sun , B. Surrow , M. Swanger , T. J. M. Symons , A. Szanto de Toledo , A. Tai , J. Takahashi , A. H. Tang , T. Tarnowsky , D. Thein , J. H. Thomas , A. R. Timmins , S. Timoshenko , M. Tokarev , T. A. Trainor , S. Trentalange , R. E. Tribble , O. D. Tsai , J. Ulery , T. Ullrich , D. G. Underwood , G. Van Buren , N. van der Kolk , M. van Leeuwen , A. M. Vander Molen , R. Varma , I. M. Vasilevski , A. N. Vasiliev , R. Vernet , S. E. Vigdor , Y. P. Viyogi , S. Vokal , S. A. Voloshin , W. T. Waggoner , F. Wang , G. Wang , J. S. Wang , X. L. Wang , Y. Wang , J. W. Watson , J. C. Webb , G. D. Westfall , A. Wetzler , C. Whitten , H. Wieman , S. W. Wissink , R. Witt , J. Wood , J. Wu , N. Xu , Q. H. Xu , Z. Xu , P. Yepes , I-K. Yoo , V. I. Yurevich , W. Zhan , H. Zhang , W. M. Zhang , Y. Zhang , Z. P. Zhang , Y. Zhao , C. Zhong , R. Zoulkarneev , Y. Zoulkarneeva , A. N. Zubarev , J. X. Zuo

We study, within the statistical hadronization model, the influence of narrow strangeness carrying baryon resonances (pentaquarks) on the understanding of particle production in relativistic heavy ion collisions. There is a great variation…

High Energy Physics - Phenomenology · Physics 2009-11-10 J. Letessier , G. Torrieri , S. Steinke , J. Rafelski

We discuss how the dynamics of the evolving hot fireball of quark--gluon matter impacts phase transition between the deconfined and confined state of matter. The rapid expansion of the fireball of deconfined matter created in heavy ion…

High Energy Physics - Phenomenology · Physics 2009-11-11 Johann Rafelski , Jean Letessier

Antiproton annihilations on nuclei provide a very interesting way to study the behaviour of strange particles in the nuclear medium. In low energy $\bar p$ annihilations, the hyperons are produced mostly by strangeness exchange mechanisms.…

Nuclear Theory · Physics 2015-06-04 A. B. Larionov , T. Gaitanos , U. Mosel

Particle production in central S-A collisions at 200 GeV/A energy is analysed within a thermal model. Present data imply that the strange particles freeze out at a higher temperature than the non-strange particles and that the strangeness…

High Energy Physics - Phenomenology · Physics 2016-08-16 E. Suhonen , J. Cleymans , K. Redlich , H. Satz

We report recent results on the dynamics of strange hadrons in two-body reactions relevant for near-threshold production in heavy-ion collisions at GSI/FAIR and NICA-Dubna. In particular, $\bar K N$ scattering in hot and dense nuclear…

High Energy Physics - Phenomenology · Physics 2016-02-17 Daniel Cabrera , Laura Tolos , Jörg Aichelin , Elena bratkovskaya

Hyperon resonances are becoming an extremely useful tool allowing the study of the properties of hadronic fireballs made in heavy ion collisions. Their yield, compared to stable particles with the same quark composition, depends on…

High Energy Physics - Phenomenology · Physics 2009-11-07 C. Markert , G. Torrieri , J. Rafelski

Using a non--relativistic gluon bound--state model for glueballs (G), we compute the subprocess $q\,\bar q\, \to\, G\,\pi$, and we therefrom derive the yield of the overall reaction $p\,\bar p\, \to\, G\,\pi X$, assuming the glueball and…

High Energy Physics - Phenomenology · Physics 2009-08-12 Francesco Murgia , Paul Kessler , Joseph Parisi

The rapid thermalization of quarks and gluons in the initial stages of relativistic heavy-ion collisions is treated using analytic solutions of a nonlinear diffusion equation with schematic initial conditions, and for gluons with boundary…

High Energy Physics - Phenomenology · Physics 2020-05-04 Georg Wolschin

The amount of proton stopping in central Pb+Pb collisions from 20-160 AGeV as well as hyperon and antihyperon rapidity distributions are calculated within the UrQMD model in comparison to experimental data at 40, 80 and 160 AGeV taken…

Nuclear Theory · Physics 2009-11-07 H. Weber , E. L. Bratkovskaya , H. Stoecker

Using a multiphase transport model, we study the production of a new strange dibaryon (\Omega\Omega)_{0+} in dense hadronic matter formed in relativistic heavy ion collisions. The (multi-)strange baryons (\Xi and \Omega) are produced by…

Nuclear Theory · Physics 2009-11-07 Subrata Pal , C. M. Ko , Z. Y. Zhang