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《中国物理C》(英文)编辑部
2024年10月30日

Thermal Freeze-Out and Longitudinally Non-uniform Collective Expansion Flow in Relativistic Heavy Ion Collisions

  • The non-uniform longitudinal flow model (NUFM) proposed recently is extended to include also the transverse flow. The resulting longitudinally non-uniform collective expansion model (NUCEM) is applied to the calculation of rapidity distribution of kaons, lambdas and protons in relativistic heavy ion collisions at CERN-SPS energies. The model results are compared with the 200A GeV/c S-S and 158 A GeV/c Pb-Pb collision data. The central dips observed in experiments are reproduced in a natural way. ;It is found that the depth of the central dip depends on the magnitude of the parameter e and the mass of produced particles, i.e. the non-uniformity of the longitudinal flow which is described by the parameter e determines the depth of the central dip for produced particles. Comparing with one-dimensional non-uniform longitudinal flow model, the rapidity distribution of lighter strange particle kaon also shows a dip due to the effect of transverse flow.
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  • [1] . Bass S A ,Gyulassy M ,St cker H et al.J.Phys.,1999,G25:R1—R57;Alber J et al.Phys.Rev.Lett.,1995,75:3814 2. Capella A ,Kopeliovich B Z .Phys.Lett.,1996,B381:325;Werner K .Phys.Rep.,1993,232:87 3. Lctessier J et al.Phys.Rev.,1995,D51:3408 4. Alber E et al(NA35 Collab.).Nucl.Phys.,1994,A566:35c;Bachler E et al(NA35 Collab.).Phys.Rev.Lett.,1994,72:1419 5. Appelshuser H et al(NA49 Collab.).Phys.Rev.Lett.,1998,80:41366. Schnedermann E ,Sollfrank J,Heinz U .Phys.Rev.,1993,C47:1738;1993,C48:2462;Schnedermann E ,Heinz U .Phys.Rev.,1994,C50:1675 7. Sollfrank J.Eur.Phys.J.,1999,C9:156;Slotta C ,SollfrankJ,HeinzU .1995 Strangenessin Hadronic Matter,AIPCon ference Proceedings 340(Wood bury:AIP process),4628. FENG ShengQin,LIU Feng,LIU LianShou.Phys.Rev.,2001,C63:014901 9. Werner K .Nucl.Phys.,1991,A525:501c;Werner K ,KochP .Phys.Lett.,1990,B242:251;Poskanzer A M ,Voloshin S A .Phys.Rev.,1998,C58:1671;Ollitrault J Y .Nucl.Phys.,1998,A638:195c 10. Gutbrod H H ,Poskanzer A M ,Ritter H G .Rep.Prog.Phys.,1989,52:1287;Gustaffson H A et al.Phys.Rev.Lett.,1984,53:1590;StckerH ,GreinerW .Phys.Rep.,1986,137:277 11. Abbott T et al.Phys.Rev.Lett.,1990,64:847;Barrette J et al(E877 Collab.).Phys.Rev.Lett.,1994,73:2543 12. Cooper H ,Frye G .Phys.Rev.,1974,D10:18613. Bjorken J D .Phys.Rev.,1983,D27:14014. Braun Munzinger P ,Stachel J,Wessels J P et al.Phys.Lett.,1995,B344:43;1996,B365:1;Braun Munzinger P ,Stachel J.Nucl.Phys.,1996,A606:320
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FENG Sheng-Qin, LIU Feng and LIU Lian-Shou. Thermal Freeze-Out and Longitudinally Non-uniform Collective Expansion Flow in Relativistic Heavy Ion Collisions[J]. Chinese Physics C, 2002, 26(12): 1277-1284.
FENG Sheng-Qin, LIU Feng and LIU Lian-Shou. Thermal Freeze-Out and Longitudinally Non-uniform Collective Expansion Flow in Relativistic Heavy Ion Collisions[J]. Chinese Physics C, 2002, 26(12): 1277-1284. shu
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Received: 2002-01-30
Revised: 1900-01-01
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Thermal Freeze-Out and Longitudinally Non-uniform Collective Expansion Flow in Relativistic Heavy Ion Collisions

    Corresponding author: FENG Sheng-Qin,
  • Institute of Particle Physics, Huazhong Normal University, Wuhan 430079, China

Abstract: The non-uniform longitudinal flow model (NUFM) proposed recently is extended to include also the transverse flow. The resulting longitudinally non-uniform collective expansion model (NUCEM) is applied to the calculation of rapidity distribution of kaons, lambdas and protons in relativistic heavy ion collisions at CERN-SPS energies. The model results are compared with the 200A GeV/c S-S and 158 A GeV/c Pb-Pb collision data. The central dips observed in experiments are reproduced in a natural way. ;It is found that the depth of the central dip depends on the magnitude of the parameter e and the mass of produced particles, i.e. the non-uniformity of the longitudinal flow which is described by the parameter e determines the depth of the central dip for produced particles. Comparing with one-dimensional non-uniform longitudinal flow model, the rapidity distribution of lighter strange particle kaon also shows a dip due to the effect of transverse flow.

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