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Maya Shimomura

Publications and source records attributed to Maya Shimomura.

2 recordsLinked to original sources

System Size and Collision Energy Dependence of $v_2$ for Identified Charged Hadrons at RHIC-PHENIX

The transverse momentum ($p_{\rm T}$) and centrality dependence of the azimuthal anisotropy ($v_{2}$) are measured for charged hadrons in different energies and collision species by the PHENIX experiment at RHIC. We find that $v_{2}$ divided by the participant eccentricity of the initial geometry proportionally increases with the number of participants to the 1/3 power except at small $N_{\rm part}$ in Cu+Cu at $\sqrt{s_{\rm NN}}$ = 62.4 GeV. Taking the eccentricity and quark number scaling into account, there is a universal scaling for $v_{2}$ with different energies and collision sizes. The results indicate that $v_{2}$ is determined by more than just the geometrical eccentricity. It also depends on the size of collision. We also report that both the behaviors of $v_{2}$ and $p_{\rm T}$ distributions can be understood from the thermal nature of produced particles based on hydro-dynamical behavior.

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High-pT pi0, eta, Identified and Inclusive Charged Hadron Spectra from PHENIX

PHENIX has extended the measurement of the pi0, eta, identified and inclusive charged hadron up to 20 GeV/c, and extended the measurement to the Cu+Cu collision system. A strong suppression is observed for both pi0 and charged hadron yields in central Au+Au and Cu+Cu collisions. Comparing Au+Au and Cu+Cu systems, RAA becomes independent of pT above 5 GeV/c. Its centrality dependence is compared with two models in order to test for universal Npart scaling that is independent of system; results are inconclusive. The results are compatible with energy loss predictions. In addition, the ratio of eta to pi0 approaches, within uncertainties, a constant value of 0.4-0.5 at high pT in p+p, d+Au, and Au+Au, while the ratio of Ks to pi0 is also consistent with a constant value at high pT in d+Au and p+p. These results are compatible with normal jet fragmentation.

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