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不同味夸克产生的喷注硬度特性的比较研究.ppt
Scaling properties of multiplicity fluctuations in heavy-ion collisions simulated by AMPT model Yi-Long Xie China University of Geosciences, Wuhan (Xie Yi-Long, Chen Gang,et al,Nucl. Phys. A 920 (2013) 33–44) Content Nonlinear Dynamics AMPT model Results of NFM Analysis Discussion of FM’s Scaling Summary China University of Geosciences School of mathematics and physics 1. Nonlinear Dynamics Big local fluctuation implied dynamical factors. China University of Geosciences School of mathematics and physics Bialas:describe the fluctuation with NFM as follow: 1. Nonlinear Dynamics China University of Geosciences School of mathematics and physics Self-similar Fractal Self-affine Fractal Criterion for existence of fractal 1. Nonlinear Dynamics China University of Geosciences School of mathematics and physics Characterize of Self-similar Fractal: Characterize of Self-affine Fractal Isotropic partition the phase-space Anisotropic partition the phase-space with calculated Hurst exponent Fitting the 1-d NFM with saturation exponents Calculate the Hurst exponent with saturation exponent Wu Y F, Liu L S. Phys Rev Lett, 1993, 70(21):3197-3200 collision at region 1. Nonlinear Dynamics Self-similar Fractal China University of Geosciences School of mathematics and physics Self-affine Fractal Hadron collision Agababyan N M, Atayan M R, Charlet M, et al. Phys Lett B, 1996, 382(3):305-311 Abreu P, Adam W, Adye T, et al. Nucl Phys B, 1992, 386(2):471-492 The final state system in collisions at region is self-affine fractal 1. Nonlinear Dynamics China University of Geosciences School of mathematics and physics The final state system in hadron collisions is self-affine fractal Does fractal exist in heavy ion collisions? Which kind of fractal? Experiments has shown that: So: A Pictorial View of Micro-Bangs at RHIC: 1. Initial Condition 2. Partonic Cascade 3. Hadronization 4. Hadronic Rescattering 2 AMPT model 2 AMPT model
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