[PDF]    https://doi.org/10.3952/physics.v57i4.3598

Open access article / Atviros prieigos straipsnis

Lith. J. Phys. 57, 201–206 (2017)


INVESTIGATING THE “KINK” PLOT AS A SIGNAL OF THE ONSET OF DECONFINEMENT
Michał Naskręta,b (for the NA61/SHINE collaboration)
aInstitute of Theoretical Physics, pl. Maxa Borna 9, 50-204 Wrocław, Poland
bNA61/SHINE collaboration, CERN, Geneva, Switzerland
michal.naskret@uwr.edu.pl

Received 12 April 2017; revised 20 June 2017; accepted 20 September 2017

One of the physics goals of the NA61/SHINE collaboration at the CERN Super Proton Synchrotron is to study the phase diagram of hadronic matter. To this end, a series of heavy ion collision measurements are performed. It is believed that above a certain collision energy and system size a phase transition between the hadronic matter and quark–gluon plasma occurs. A number of observables have been developed to determine which of the phases was created at the early stage of the collision. This report discusses the dependence of the ratio of the mean number of produced pions to the mean number of wounded nucleons on the Fermi energy measure. For comparison with other measurements this is often presented in the form of the “kink” plot. This plot is presented enriched with preliminary results for 40Ar+45Sc central collisions at 13A, 19A, 30A, 40A, 75A and 150A GeV/c beam momenta. The results are finally compared to data from other experiments.
Keywords: NA61/SHINE, CERN, quark–gluon plasma, onset of deconfinement
PACS: 25.75.-q, 25.75.Nq

„PŪPSNIO“ GRAFIKO KAIP SIGNALO APIE KVARKŲ IŠLAISVĖJIMO PRADŽIĄ TYRIMAS
Michał Naskręta,b (už NA61/SHINE sambūrį)

aTeorinės fizikos institutas, Vroclavas, Lenkija
bNA61/SHINE samburis, CERN, Ženeva, Šveicarija


References / Nuorodos

[1] N. Abgrall, O. Andreeva, A. Aduszkiewicz, Y. Ali, T. Anticic, N. Antoniou, B. Baatar, F. Bay, A. Blondel, J. Blumer, et al., NA61/SHINE facility at the CERN SPS: beams and detector system, J. Instrum. 9, P06005 (2014),
https://doi.org/10.1088/1748-0221/9/06/P06005
[2] M. Gell-Mann, A schematic model of baryons and mesons, Phys. Lett. 8, 214–215 (1964),
https://doi.org/10.1016/S0031-9163(64)92001-3
[3] G. Zweig, An SU(3) model for atrong interaction symmetry and its breaking, CERN Report No. 8182/TH.401 (1964),
http://inspirehep.net/record/11881?ln=en
[4] J.C. Collins and M.J. Perry, Superdense matter: Neutrons or asymptotically free quarks? Phys. Rev. Lett. 34, 1353 (1975),
https://doi.org/10.1103/PhysRevLett.34.1353
[5] M. Gaździcki and M.I. Gorenstein, On the early stage of nucleus–nucleus collisions, Acta Phys. Pol. B 30, 2705–2735 (1999),
http://www.actaphys.uj.edu.pl/vol30/abs/v30p2705
[6] A. Białas, M. Bleszyński, and W. Czyż, Multiplicity distributions in nucleus–nucleus collisions at high energies, Nucl. Phys. B 111(3), 461–476 (1976),
https://doi.org/10.1016/0550-3213(76)90329-1
[7] K. Werner, F.-M. Liu, and T. Pierog, Parton ladder splitting and the rapidity dependence of transverse momentum spectra in deuteron–gold collisions at the BNL Relativistic Heavy Ion Collider, Phys. Rev. C 74, 044902 (2006),
https://doi.org/10.1103/PhysRevC.74.044902
[8] N. Abgrall, A. Aduszkiewicz, Y. Ali, T. Anticic, N. Antoniou, B. Baatar, F. Bay, A. Blondel, J. Blumer, M. Bogomilov, et al., Measurement of negatively charged pion spectra in inelastic p+p interactions at plab = 20, 31, 40, 80 and 158 GeV/c, Eur. Phys. J. C 74(3), 2794 (2014),
https://doi.org/10.1140/epjc/s10052-014-2794-6
[9] M. Rybczyński, G. Stefanek, W. Broniowski, and P. Bozek, GLISSANDO 2: GLauber Initial-State Simulation AND mOre..., ver. 2, Comput. Phys. Commun. 185(6), 1759–1772 (2014),
https://doi.org/10.1016/j.cpc.2014.02.016
[10] C. Patrignani, K. Agashe, G. Aielli, C. Amsler, M. Antonelli, D.M. Asner, H. Baer, S. Banerjee, R.M. Barnett, T. Basaglia, et al. (Particle Data Group), Review of Particle Physics, Chin. Phys. C 40(10), 100001 (2016),
https://doi.org/10.1088/1674-1137/40/10/100001
[11] G. Baym, Confinement of quarks in nuclear matter, Phys. A 96(1), 131–135 (1979),
https://doi.org/10.1016/0378-4371(79)90200-0