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Anti-flow of K$^0_s$ Mesons in 6 AGeV Au + Au Collisions

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arxiv nucl-ex/0101003 v1 pith:ZENPJBSZ submitted 2001-01-06 nucl-ex

P.Chung , N.N.Ajitanand , J.M.Alexander , M.Anderson , D.Best , F.P.Brady , T.Case , W.Caskey
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D.Cebra J.L.Chance B.Cole K.Crowe A.Das J.E.Draper M.L.Gilkes S.Gushue M.Heffner A.S.Hirsch E.L.Hjort L.Huo M.Justice M.Kaplan D.Keane J.C.Kintner J.Klay D.Krofcheck R.A.Lacey J.Lauret M.A.Lisa H.Liu Y.M.Liu R.McGrath Z.Milosevich G.Odyniec D.L.Olson S.Y.Panitkin C.Pinkenburg N.T.Porile G.Rai H.G.Ritter J.L.Romero R.Scharenberg L.Schroeder B.Srivastava N.T.BStone T.J.M.Symons T.Wienold R.Witt J.Whitfield L.Wood W.N.Zhang
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keywords agevanti-flowcollisionsmattermesonsnuclearcentralcross
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abstract

We have measured the sideward flow of neutral strange ($K^0_s$) mesons in 6 AGeV Au + Au collisions. A prominent anti-flow signal is observed for an impact parameter range (b $\lesssim 7$ fm) which spans central and mid-central events. Since the $K^0_s$ scattering cross section is relatively small in nuclear matter, this observation suggests that the in-medium kaon vector potential plays an important role in high density nuclear matter.

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Cited by 1 Pith paper

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  1. Impact of particle production mechanisms on pseudorapidity distribution and directed flow in Au+Au and Cu+Cu collisions at $\sqrt{s_{NN}}$ = 19.6 GeV using AMPT model

    nucl-th 2025-06 conditional novelty 4.0 of 10

    String fragmentation parameters in the AMPT model change proton directed flow and its system-size dependence at 19.6 GeV, while leaving pions nearly unaffected.

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