Abstract

We present measurements of azimuthal correlations of charged hadron pairs in $\sqrt{s_{_{NN}}}=200$ GeV Au$+$Au collisions for the trigger and associated particle transverse-momentum ranges of $1<p_T^t<10$~GeV/$c$ and $0.5<p_T^a<10$~GeV/$c$. After subtraction of an underlying event using a model that includes higher-order azimuthal anisotropy $v_2$, $v_3$, and $v_4$, the away-side yield of the highest trigger-\pt ($p_T^t>4$~GeV/$c$) correlations is suppressed compared to that of correlations measured in $p$$+$$p$ collisions. At the lowest associated particle $p_T$ ($0.5<p_T^a<1$ GeV/$c$), the away-side shape and yield are modified relative to those in $p$$+$$p$ collisions. These observations are consistent with the scenario of radiative-jet energy loss. For the low-$p_T$ trigger correlations ($2<p_T^t<4$ GeV/$c$), a finite away-side yield exists and we explore the dependence of the shape of the away-side within the context of an underlying-event model. Correlations are also studied differentially versus event-plane angle $\Psi_2$ and $\Psi_3$. The angular correlations show an asymmetry when selecting the sign of the difference between the trigger-particle azimuthal angle and the $\Psi_2$ event plane. This asymmetry and the measured suppression of the pair yield out of plane is consistent with a path-length-dependent energy loss. No $\Psi_3$ dependence can be resolved within experimental uncertainties.

Highlights

  • The PHENIX detector [65] was designed to measure charged hadrons, leptons, and photons to study the nature of the quark gluon plasma (QGP) formed in ultrarelativistic heavy-ion collisions

  • Charged hadron tracks are reconstructed in the PHENIX central arm spectrometer (CNT), which is comprised of two separate arms, east and west

  • The results presented are based on an analysis lion minimum-bias events for Au + Au collisions of at

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Summary

INTRODUCTION

Energy loss of hard-scattered partons (jet quenching [1]) resulting from the interaction of a colored parton in the quark gluon plasma (QGP) formed in relativistic heavy-ion collisions at the Relativistic Heavy Ion Collider (RHIC) [2,3,4,5]. Observations of the energy-loss effects mentioned above, especially for lower jet and particle momenta in two-particle correlations, have been obscured due to the much larger contribution from the underlying event at these momenta. Varying the path length by selecting azimuthal orientations relative to the second-order event plane has been explored for single-particle or single-jet observables at high pT [11,64]. Such differential correlations probe the path-length and geometrical dependence of energy loss with more event-by-event sensitivity and extend similar studies of high-pT correlations [16] down to lower pT.

PHENIX DETECTOR
Particle selection
Event plane and resolution
Two-particle correlations
Inclusive trigger correlations Two-particle correlations are calculated as
Event-plane-dependent correlations
Flow background model including event-plane dependence
42. We estimate
PHENIX
Unfolding of event-plane-dependent correlations
Iterative Bayesian unfolding
Fourier oscillation correction of event-plane-dependence of correlations
Efficiency
Inclusive per-trigger yields
Event-plane-dependent per-trigger yields
Inclusive per-trigger yields I
Inclusive per-trigger yields II
SUMMARY
Methods
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