The initial and final temperatures in some high energy collisions

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Presentation transcript:

The initial and final temperatures in some high energy collisions Reporter : Qi Wang(王琪) Supervisor : Fu-Hu Liu(刘福虎) The 18th national congress on medium and high energy nuclear physics(2019.6.21)

Outline Results and discussion Formalism and method Background Summary and conclusion

Background Distribution of transverse momentum The hagedorn function(inverse power-law) The initial state temperature The final state temperature The Erlang distribution Distribution of transverse momentum The blast-wave model The simplest standard distribution The simplest Boltzmann distribution

Background The Erlang distribution Analysis of transverse momentum spectra The Erlang distribution (the folding of n exponential functions) The initial state temperature

Boltzmann-Gibbs statistics Background Analysis of transverse momentum spectra Blast-wave model The final state temperature Boltzmann-Gibbs statistics Tsallis statisics

Background The comparisons between a few distributions of transverse momenta are useful to understand carefully different distributions in high energy collisions. The excitation functions of the initial and final state temperatures are very interesting for us to study the properties of high energy collisions. Although there are many similar studies on this topic, the results seem to be inconsistent.

Formalism and method The hagedorn function( inverse power-law ) and its modified forms R. Odorico, Phys. Lett. B 118, 151 (1982). K.Aamodt et al.(ALICE Collaboration) Phys. Lett. B 693, 53 (2010). A.De Falco (for the ALICE Collaboration) J. Phys. G 38, 124083 (2011). B.Abelev et al.(ALICE Collaboration) Phys. Lett. B 708,265 (2012).

E. Schnedermann, J. Sollfrank, U. W. Heinz Formalism and method The simplest standard distribution and its modified forms J. Cleymans, D. Worku Eur. Phys. J. A 48, 160 (2012). E. Schnedermann, J. Sollfrank, U. W. Heinz Phys. Rev. C 48, 2462 (1993). H. Zhao, F.-H. Liu Adv.High Energy Phys. 2014, 742193 (2014).

Formalism and method The simplest Boltzmann distribution and its modified forms J. Cleymans, D. Worku, Eur. Phys. J. A 48, 160 (2012).

F.-H. Liu, J.-S. Li, Phys. Rev. C 78, 044602 (2008). Formalism and method The Erlang distribution The initial state temperature F.-H. Liu, J.-S. Li, Phys. Rev. C 78, 044602 (2008). [1] Gutay L G, Hirsch A S, Pajares C, Scharenberg R P and Srivastava B K 2015 Int. J. Mod. Phys. E 24 1550101. [2] Hirsch A S, Pajares C, Scharenberg R P and Srivastava B K 2018 (arXiv:1803.02301 [hep-ph]).

Formalism and method The blast-wave fit Boltzmann-Gibbs statistics Tsallis statistics E. Schnedermann, J. Sollfrank, U. Heinz Phys. Rev. C 48, 2462 (1993) Z.B. Tang, Y.C. Xu, L.J. Ruan, G. van Buren, F.Q. Wang, Z.B. Xu, Phys. Rev. C 79, 051901(R) (2009).

Formalism and method The blast-wave fit The boost angle G. Agakishiev et al. (STAR Collaboration), Identified hadron compositions in p+p and Au+Au collisions at high transverse momenta at . Phys. Rev. Lett. 108, 072302 (2012). https://doi.org/10.1103/PhysRevLett.108.072302 The blast-wave fit The boost angle The self-similar flow profile The transverse flow velocity The final state temperature T0

Results and discussion The experiental data Collabration Particles Energy STAR Au+Au 7.7, 11.5, 19.6, 27, 36, 62.4, 130 GeV LHCB p+He 110 GeV STAR/PHENIX 200 GeV d+Au ALICE Pb+Pb 2.76 TeV

Results The hagedorn function( inverse power-law ) and its modified forms

Results The simplest standard distribution and its modified forms

Results The simplest Boltzmann distribution and its modified forms

Results The Erlang distribution, the inverse power-law and blast-wave model

Results The Erlang distribution, the inverse power-law and blast-wave model

Results Dependences of parameters on energy in different centrality intervals

Results Dependences of parameters on centrality at different energies

Summary and conclusion For the Hagedorn function, the effect of rest mass in the first modified form is very small due to large transverse momentum. The other two modified forms describe narrow transverse momentum range. For the simplest standard and Boltzmann distributions, the modified forms contribute a wider transverse momentum range than the original distributions. The excitation functions of show a drop at 27 GeV, and an increase from dozens of GeV to 2.76 TeV. The excitation functions of show an increase from 7.7 GeV to 2.76 TeV. The mean transverse momentum and the initial state temperature increase approximately linearly with the increase of logarithmic collision energy. It is a long-term target to search for the relation between the value of prameter and logarithmic collision energy.

Thank for your attention! This work was supported by the National Natural Science Foundation of China under Grant Nos.11575103 and 11747319, the Shanxi Provincial Natural Science Foundation under Grant No. 201701D121005, and the Fund for Shanxi “1331 Project” Key Subjects Construction.