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Yoki Aramaki

Publications and source records attributed to Yoki Aramaki.

3 recordsLinked to original sources

First measurement of $\phi$ meson production in 30 GeV proton-nucleus reactions via di-electron decay at J-PARC

We present the first measurement of the production of the $\phi$ meson in 30 GeV proton-nucleus interactions on carbon and copper targets via the di-electron decay channel. The measurement was conducted at the high-momentum beamline of the J-PARC Hadron Experimental Facility, which was commissioned in 2020. The $e^+e^-$ pairs were detected using the E16 spectrometer, during a commissioning run of the J-PARC E16 experiment. The $\phi$ mesons are successfully reconstructed on all experimental targets. The obtained yields are converted to the total production cross section, assuming a kinematical distribution of the event generator JAM. The total cross sections derived are 2.0 $\pm$ 0.9 (stat.) $\pm$ 1.0 (syst.) mb on the carbon target and 10.3 $\pm$ 4.4 (stat.) $\pm$ 4.4 (syst.) mb on the copper target. The mass-number dependence of the cross section is discussed using the parameter $\alpha$, defined as $\sigma \propto A^\alpha$, resulting in $\alpha = $ 0.99 $\pm$ 0.38 (stat.) $\pm$ 0.34 (syst.). The extrapolation to $A=1$, which means that the cross section of proton-proton reactions, is in good agreement with the existing measurements at comparable energies.

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Study of QGP with probes associated with photon at RHIC-PHENIX

When heavy ions with high energy collide, a hot and dense matter is produced. As the matter expands, the matter undergoes cross-over phase transition from partonic matter to hadronic matter. Jets are created by high pT partons in the early phase of the collisions. Leptons and photons can penetrate the matter without strong interaction. For that reason, jets, leptons and photons are good probes to study the partonic matter in the early phase of the collisions. We report about two probes associated with photon and their results for PHENIX.

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Reaction plane dependence of neutral pion production in center-of-mass energy of 200 GeV Au+Au collisions at RHIC-PHENIX

It has been observed in central Au+Au collisions at Relativistic Heavy Ion Collider (RHIC) that the yield of neutral pions at high transverse momentum (pT> 5 GeV/c) is strongly suppressed compared to the one expected from p+p collisions scaled by the number of binary collisions. This suppression is considered to be due to the energy lost by hard scattered partons in the medium (jet quenching), which results in a decrease of the yield at a given pT. The magnitude of the suppression depends on the path length of scattered partons in the medium. Studying the path length dependence of energy loss should provide additional information on the energy loss mechanism in the medium. For example, some theoretical models suggest that the LPM effect in Quantum ChromoDynamics (QCD) plays an important role in radiative energy loss and predict that the magnitude of the energy loss is proportional to square of path length. We can estimate the path length by measuring the azimuthal angle from reaction plane and mapping it into the shape of the participant region, which can be calculated by Glauber model for each impact parameter (centrality). We discuss the parton energy loss using the nuclear modification factor (RAA) of neutral pion with respect to the path length. The integrated luminosity of RHIC-Year7 Au+Au run is 813 $μ$b^{-1}, which is 3.5 times larger statistics than that in RHIC-Year4 Au+Au run. Additionally, a new detector was installed to determine reaction plane more precisely. This detector is expected to provide better resolution for reaction plane determination. These advantages enable us to precisely measure the path length dependence of neutral pion suppression and discuss parton energy loss mechanism more thoroughly.

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