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High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models
High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models
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High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models
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High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models
High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models

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High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models
High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models
Journal Article

High \\(p_{\\rm T}\\) leading hadron suppression in nuclear collisions at \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV: data versus parton energy loss models

2005
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Overview
Experimental results on high transverse momentum (leading) hadron spectra in nucleus-nucleus collisions in the range \\(\\sqrt{s_{NN}}\\approx\\) 20-200 GeV are reviewed with an emphasis on the observed suppression compared to free space production in proton-proton collisions at the corresponding center-of-mass energies. The transverse-momentum and collision-energy (but seemingly not the in-medium path length) dependence of the experimental suppression factors measured in central collisions is consistent with the expectations of final-state non-Abelian parton energy loss in a dense QCD medium.