2006
DOI: 10.1140/epja/i2006-10101-2
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Systematics of stopping and flow in Au+ Au collisions

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Cited by 123 publications
(145 citation statements)
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“…Methods developed and described in Refs. [36,37] for correcting the finite dispersion of the reaction plane were applied. The coefficients v 1 and v 2 representing the strengths of directed and elliptic flows, respectively, were deduced from fits with the Fourier expansion f (∆φ ) ∝ 1 + 2v 1 cos(∆φ ) + 2v 2 cos(2∆φ ).…”
Section: Resultsmentioning
confidence: 99%
“…Methods developed and described in Refs. [36,37] for correcting the finite dispersion of the reaction plane were applied. The coefficients v 1 and v 2 representing the strengths of directed and elliptic flows, respectively, were deduced from fits with the Fourier expansion f (∆φ ) ∝ 1 + 2v 1 cos(∆φ ) + 2v 2 cos(2∆φ ).…”
Section: Resultsmentioning
confidence: 99%
“…This maximum is further supported by the nuclear stopping at 400 MeV/nucleon [70]. Beyond this energy, the elliptical flow decreases indicating a transition to preferentially in-plane emission [53,54]. This rise-and-fall behavior of the elliptical flow in the expansion region is due to the variation in the passing time of the spectator and the expansion time of the participant zone [21,22].…”
Section: The Iqmd Modelmentioning
confidence: 94%
“…The pulsating sign observed recently at intermediate energies has received particular attention, as it reflects the increased pressure build-up in the non-isotropic collision zone [45]. After the pioneering measurements at Saturne [46] and Bevalac [47], a wealth of experimental results have been obtained at Bevalac and SIS [15,[20][21][22][23][48][49][50][51][52] as well as at AGS [53,54], SPS [45], and RHIC [55]. In recent years, the FOPI, INDRA, and PLASTIC BALL Collaborations [20][21][22][23] have been actively involved in measuring the excitation function of elliptical flow from Fermi energies to relativistic ones.…”
Section: Introductionmentioning
confidence: 99%
“…However, the multiplicity of emitted particle species and the dynamic evolution of the hot and dense nuclear medium (including density and momentum) together decide the complexity and richness of the excitation function of flow results [4,22,23]. Therefore, besides the stiffness of EoS, the treatment in collision term, especially on the medium modifications of (differential) cross sections with various incoming and outcoming particle types, ought to be paid more attention.…”
Section: Urqmd Model and Collective Flowsmentioning
confidence: 99%