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Volumn 72, Issue 1, 2005, Pages

Kaon production and propagation at intermediate relativistic energies

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EID: 26944453208     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.72.014901     Document Type: Article
Times cited : (29)

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    • Notice that in Fig. 2 and Table 1 we summed up the nucleon-Δ(1232) and nucleon-higher-resonance channels, while in Fig. 4 these channels are shown separately.
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    • The parameters v1 and v2 of the fit 12 are equal to those given by Eqs. 9 and 10 within accepted accuracy up to the terms with n>2 in the Fourier expansion 8, which we neglect. Thus, we will also call the fit parameters v1 and v2 as the directed and elliptic flows, respectively. Since the azimuthal distributions are extracted at midrapidity, the directed flow v1 should be equal to zero for symmetry reasons. We obtained v1~10-3 in the fitting procedure due to finite statistics, which is much smaller than the extracted values of |v2|. Thus, we drop the explicit values of the v1 coefficient.
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