Abstract

We present empirical features of parton energy loss in nucleus–nucleus collisions at RHIC through studies of the spectra and nuclear modification factors ( R A A ) for charged hadrons, neutral pions ( π 0 ) and non-photonic electrons. The flat distribution of R A A at high transverse momentum ( p T ) for a given collision centrality is consistent with a scenario where parton energy loss Δ p T is proportional to p T . The centrality dependence of the parton energy loss indicates the absence of path length dependence in the magnitude of energy loss. The lack of strong path length dependence suggests a dynamical picture where the dense partonic medium undergoes rapid expansion and the density of the medium falls rapidly in the first a few Fermi interval, which may be much shorter than the full path length. Implications of the empirical constraints on the parton energy loss will also be discussed.

Highlights

  • Nucleus-nucleus collisions at RHIC produce a hot and dense medium

  • Particle production in the higher pT region is consistent with features of parton fragmentations, and may be used to study parton energy loss in the hot and dense medium

  • Experimental measurements at RHIC have shown a strong suppression of high pT particles with respect to the expectation of binary nucleon-nucleon collision scaling for charged hadrons [3], for neutral pions [4, 5] and for non-photonic electrons [6]

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Summary

If we assume the linear dependence on and

Both approximately proportional to the cube root number of participants (Npart), the energy loss goes with Np2a/r3t as observed for π0 by the experimentally measured dN dy. If the collision system S, and L by dN g

Npart and
Fractional energy loss
We note that the observed
The RAA
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