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PHENIX Measurement of Charged Kaon Interferometry in Au+Au Collisions at s NN = 200 GeV

PHENIX Measurement of Charged Kaon Interferometry in Au+Au Collisions at s NN = 200 GeV. APS-JPS Joint meeting at Maui, Hawaii, Sep. 22 th 2005. Akitomo Enokizono Lawrence Livermore National Laboratory.  UCRL-PRES-215491

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PHENIX Measurement of Charged Kaon Interferometry in Au+Au Collisions at s NN = 200 GeV

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  1. PHENIX Measurement of Charged Kaon Interferometry in Au+Au Collisionsat sNN=200 GeV APS-JPS Joint meeting at Maui, Hawaii, Sep. 22th 2005 Akitomo Enokizono Lawrence Livermore National Laboratory  UCRL-PRES-215491 This work was performed under the auspices of the U.S. Department of Energy by University of California, Lawrence Livermore National Laboratory under Contract W-7405-Eng-48.

  2. Physics interests in kaon HBT (Outline) • Are there differences of HBT radii between pion and kaon? • Different x-p correlation, freezeout time? (different Rside, Rlong?) • Different opacity to the outward direction? (larger Rout than that of pion?) • Measurements of kaon HBT radii and comparison with those of pion give us a detailed insight into a relation between source dynamics and HBT radii. • How is it predicted by Hydrodynamics models? • An important step to get information to solve HBT-puzzle. • Does kaon emission source function has “non-Gaussian” structure, which has been observed for pion 1-D HBT imaging? • We don’t know where the non-Gaussian structure of pion source come from. ( Core-halo structure due to long resonances? Just a kinetically oblong source?) • Kaon HBT-imaging analysis could clarify it.

  3. Measurement of charged kaon pairs by PHENIX • ~600M good events from PHENIX Run4 at Au+Au 200 GeV.( |Zvertex|<30cm ) • Centrality is determined by BBC-ZDC correlation • Charged hadrons tracks are reconstructed ed with DCH, EMCal, PC1,3. ( ||<0.35, =90 ) • Charged hadrons within 2 within kaon mass but 3 away from pion and proton masses are identified as charged kaons. ( 0.3<p<2.0 GeV/c ) Total pair statistics : K+K+ ~15M, K-K- ~14M (This talk shows results from K+K++K-K- of ~29M ) are measured for kT = 0.3-0.65, 0.65-0.9, 0.9-2.0 GeV/c Centrality = 0-10, 10-20, 30-93% (Each has ~10M K+K++K-K- pairs.)

  4. Reminder: Bertsch-Pratt parameterization Assuming cylindrical source and longitudinally center of mass frame. observer Rside Beam axis Rout Rlong Rout Rside Au Au Beam axis observer Rout/Rside emission duration, source opacity, kinetics… Sinyukov fit

  5. Pair momentum dependence of C2 (K+K+ + K-K-) PHENIX Preliminary K+K++K-K- (Au+Au 200 GeV )

  6. Au+Au at 200 GeV (0-30% centrality) (Run4) K+K+ + K-K- Sys.Err. ++ -- (Run2) Sys.Err. mT dependence of HBT radii PHENIX Preliminary

  7. Centrality dependence C2 (K+K+ + K-K-) PHENIX Preliminary K+K++K-K- (Au+Au 200 GeV)

  8. Au+Au 200 GeV (0.3<kT<2.0 GeV/c) Au+Au 200 GeV (0.3<kT<2.0 GeV/c) PHENIX Preliminary PHENIX Preliminary (Run4) (Run4) K+K+ + K-K- K+K+ + K-K- Sys.Err. Sys.Err. ++ ++ -- -- (Run2) (Run2) Sys.Err. Sys.Err. <mT>~0.47 (<kT>~0.45) <mT>~0.89 (<kT>~0.88) All pion HBT radii are rescaled from <mT> = 0.47 to 0.89 GeV/c Pion <mT>~0.47 GeV rescale Kaon <mT>~0.89 GeV Npart dependence of HBT radii (K+K+ + K-K-)

  9. (Run4) K+K+ + K-K- Sys.Err. ++ -- (Run2) Sys.Err. mT and Npart dependence of Rout/Rside PHENIX Preliminary PHENIX Preliminary Au+Au at 200 GeV (0.2<kT<3.0 GeV/c) Au+Au at 200 GeV (0-30% centrality) Rside and Rout are rescaled from <mT> = 0.47 to 0.89 GeV/c Rout/Rside of kaon is systematically higher than that of pion at the central collision but consistent within errors.

  10. Au+Au at 200 GeV (0-30% centrality) K+K+ + K-K- (Run4) Sys.Err. ++ -- (Run2) Sys.Err. Hydro+UrQMD – kaon Hydro+UrQMD – pion (S. Soff, nucl-th/0202240, Tc=160MeV) Theoretical mT dependence of kaon HBT radii PHENIX Preliminary PHENIX Preliminary Final rescattering effect should be negligible?

  11. HBT-imaging analysis is kernel which can be calculated from BEC and known final state interactions of pairs. is source function which represents the emission probability of pairs at r in the pair CM frame. S(r) is expanded in a function basis. Imaging by minimization of 2 Most probable source function is D.A. Brown and P. Danielewicz Phys. Rev. C. 64, 014902 (2001)

  12. 1-D kaon (K+K++K-K-) imaging PHENIX Preliminary PHENIX Preliminary Au+Au 200 GeV, 0.3<kT<2.0 GeV/c 0-30% centrality Au+Au 200 GeV, 0.3<kT<2.0 GeV/c 0-30% centrality

  13. Summary 3-D Bose-Einstein correlations for charged kaon pairs are analyzedusing Run4 PHENIX data (~600M) at Au+Au 200 GeV. • Kaon HBT radii (Rside, Rout, Rlong) well agree with those of pion as a function of transverse mass momentum (mT). • The number of participants dependence of Rside, Rout, Rlong also agree with those of pion after rescaling them to the same <mT>. • Probably there is no differences of x-p correlation and freezeout time between charged pions and kaons at the same mT and Npart region. • Rout/Rside at central collision shows systematically a bet larger value (~1.1-1.3), but still consistent with unity and pions within errors. • Comparison with hydrodynamics prediction maybe hint at small final rescattering effect. • 1-D source function by kaon imaging analysis shows a deviation from Gaussian shape, but consistent within large systematic errors. !Need a work to minimize systematic errors!

  14. Backup slides

  15. K+K+ K-K- (Run4) ++ -- (Run2) mT dependence of HBT radii (K+K+ and K-K-) PHENIX Preliminary

  16. K+K+ K-K- (Run4) ++ -- (Run2: <mT> rescaled) Npart dependence of HBT radii (K+K+ and K-K- ) PHENIX Preliminary

  17. 1-D kaon (K+K+ and K-K-) imaging results PHENIX Preliminary PHENIX Preliminary Au+Au 200 GeV, 0.3<kT<2.0 GeV/c 0-30% centrality Au+Au 200 GeV, 0.3<kT<2.0 GeV/c 0-30% centrality

  18. Systematic errors *Unit is in percentage.

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