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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

The phenomenological approach in the framework of Quark-Gluon String Model (QGSM) has been applied to the description of transverse momentum spectra for the baryon production at colliders. The analysis of data on hyperon transverse momentum…

High Energy Physics - Phenomenology · Physics 2018-11-12 Olga I. Piskounova

We evaluate the strangeness production from equilibrating and transversely expanding quark gluon plasma which may be created in the wake of relativistic heavy ion collisions. We consider boost invariant longitudinal and cylindrically…

Nuclear Theory · Physics 2009-11-07 Dipali Pal , Abhijit Sen , Munshi G. Mustafa , Dinesh K. Srivastava

The production of strange hadrons (K$^{0}_{\rm S}$, $\Lambda$, $\Xi^{\pm}$, and $\Omega^{\pm}$), baryon-to-meson ratios ($\Lambda/{\rm K}^0_{\rm S}$, $\Xi/{\rm K}^0_{\rm S }$, and $\Omega/{\rm K}^0_{\rm S}$), and baryon-to-baryon ratios…

Nuclear Experiment · Physics 2023-10-02 ALICE Collaboration

This is a short survey of signatures and characteristics of the quark-gluon plasma in the light of experimental results that have been obtained over the past three decades. In particular, we present an in-depth discussion of the strangeness…

Nuclear Theory · Physics 2017-11-01 Peter Koch , Berndt Müller , Johann Rafelski

Due to its large acceptance, the STAR experiment has acquired a wealth of data on strangeness production for a variety of collisions systems and energies, from p+p to Au+Au. By using the yields and spectra, we address the evolution of the…

Nuclear Experiment · Physics 2010-12-17 Matthew A. C. Lamont

The aim of this paper is to investigate the effect of a non-extensive form of statistical mechanics proposed by Tsallis on the formation of a quark-gluon plasma (QGP). We suggest to account for the effects of the dominant part of the…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. M. Teweldeberhan , H. G. Miller , R. Tegen

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

The increase of strange-particle yields relative to pions versus charged-particle multiplicity in proton-proton (pp) collisions at the LHC is usually described by microscopic or hydrodynamical models as a result of the increasing density of…

High Energy Physics - Phenomenology · Physics 2021-09-14 Constantin Loizides , Andreas Morsch

The recent developments in the search of exotic pentaquark hadrons are briefly reviewed. We then focus on investigating how the exotic pentaquark $\Theta(1540)$ baryon production can be identified in the $\gamma N \to K \bar{K} N$…

High Energy Physics - Phenomenology · Physics 2009-11-10 Yongseok Oh , K. Nakayama , T. -S. H. Lee

Based on a multi-phase transport model for relativistic heavy-ion collisions, effects of the parton scatterings on the production of strangeness in relativistic heavy-ion collisions are studied. It is found that the distributions of strange…

Nuclear Theory · Physics 2023-07-06 Gao-Chan Yong

The experimental data on p, Lambda, Xi-, Omega-, baryons and the corresponding antibaryons spectra obtained by different collaborations are compared with the results of the calculations performed into the frame of the Quark-Gluon String…

High Energy Physics - Phenomenology · Physics 2016-02-17 G. H. Arakelyan , C. Merino , Yu. M. Shabelski

The effect of the non-extensive form of statistical mechanics proposed by Tsallis on the formation of a quark-gluon plasma (QGP) has been recently investigated in ref. \cite{1}. The results show that for small deviations ($\approx 10%$)…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. M. Teweldeberhan , H. G. Miller , R. Tegen

The production of ${\rm\Xi}^-$ and ${\rm\Omega}^-$ baryons and their anti-particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV has been measured using the ALICE detector. The transverse momentum spectra at mid-rapidity ($|y| <…

Nuclear Experiment · Physics 2014-09-17 ALICE Collaboration

Experimental findings of recent years blurred the frontier between large and small systems. The features attributed to the Quark Gluon Plasma formation have also been found in smaller systems when measuring particle production in high…

High Energy Physics - Experiment · Physics 2024-01-26 Nicolò Jacazio

The energy dependence of the reactions pp -> p Lambda K+ and pp -> p Sigma0 K+ and the ratio R(Lambda/Sigma0} is studied in a constituent quark-gluon model, including the excitation of the baryon resonances N*(1650), N*(1710) and N*(1720)…

Nuclear Theory · Physics 2007-05-23 M. Dillig , M. Schott

We address the flavour composition along the border between the hadronic and the quark-gluon plasma phases of QCD. The ratio of strange to up and down antiquarks ($\lambda_s$) produced in partic le and nuclear collisions, is found to…

High Energy Physics - Phenomenology · Physics 2010-05-28 Sonja Kabana

A recent paper on energy dependence of strangeness production in A+A and p+p interactions written by Dunlop and Ogilvie (Phys. ReV. C61 031901(R) (2000) indicates that there is a significant misunderstanding about the concept of strangeness…

High Energy Physics - Phenomenology · Physics 2016-09-06 Marek Gazdzicki , Mark I. Gorenstein , Dieter Roehrich

We calculate saturation curves for strange hadron matter using recently constructed baryon-baryon potentials which are constrained by SU(3) symmetry. All possible interaction channels within the baryon octet (consisting of $N$, $\Lambda$,…

Nuclear Theory · Physics 2009-10-31 V. G. J. Stoks , T. -S. H. Lee

This is a critical review of the various observables that have been proposed to signal the change from dense hadronic matter to a quark-gluon plasma at high temperature or baryon density. I discuss current models of quark-gluon plasma…

Nuclear Theory · Physics 2014-11-18 Berndt Mueller
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