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A Description of the Transverse Momentum Distributions of Charged Particles Produced in Heavy Ion Collisions at RHIC and LHC Energies

Jiaqi HuiCollege of Science, University of Shanghai for Science and Technology, Shanghai 200093, ChinaZhi-Jin JiangCollege of Science, University of Shanghai for Science and Technology, Shanghai 200093, ChinaD. XuCollege of Science, University of Shanghai for Science and Technology, Shanghai 200093, China
2018en
ABI

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By assuming the existence of memory effects and long-range interactions, nonextensive statistics together with relativistic hydrodynamics including phase transition are used to discuss the transverse momentum distributions of charged particles produced in heavy ion collisions. It is shown that the combined contributions from nonextensive statistics and hydrodynamics can give a good description of the experimental data in Au+Au collisions at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M1"><mml:msqrt><mml:msub><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn fontstyle="italic">200</mml:mn></mml:math> GeV and in Pb+Pb collisions at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M2"><mml:msqrt><mml:msub><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn fontstyle="italic">2.76</mml:mn></mml:math> TeV for <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M3"><mml:mrow><mml:msup><mml:mrow><mml:mi>π</mml:mi></mml:mrow><mml:mrow><mml:mo>±</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M4"><mml:mrow><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>±</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math> in the whole measured transverse momentum region and for <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M5"><mml:mi>p</mml:mi><mml:mfenced separators="|"><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mo>-</mml:mo></mml:mover></mml:mrow></mml:mfenced></mml:math> in the region of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M6"><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>≤</mml:mo><mml:mn fontstyle="italic">2</mml:mn><mml:mo>.</mml:mo><mml:mn fontstyle="italic">0</mml:mn></mml:math> GeV/c. This is different from our previous work using the conventional statistics plus hydrodynamics, where the describable region is only limited in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="M7"><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>≤</mml:mo><mml:mn fontstyle="italic">1.1</mml:mn></mml:math> GeV/c.

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