Abstract <p>The properties of the quark-gluon medium formed in Cu + Au collisions at an energy of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\sqrt {{{s}_{{NN}}}} \)</EquationSource> <!--PhysPart2570123Basirov-m3--> </InlineEquation> = 200 GeV can be investigated using information on the energy loss of high-energy partons (<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({{p}_{{\text{T}}}} \gg {{\Lambda }_{{{\text{QCD}}}}}\)</EquationSource> <!--PhysPart2570123Basirov-m4--> </InlineEquation>). One of the quantities that can be estimated experimentally is the fractional parton energy loss <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({{S}_{{{\text{loss}}}}}\)</EquationSource> <!--PhysPart2570123Basirov-m5--> </InlineEquation>. On the basis of the data on the elliptic flow <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({{v}_{2}}\)</EquationSource> <!--PhysPart2570123Basirov-m6--> </InlineEquation> of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({{\pi }^{0}}\)</EquationSource> <!--PhysPart2570123Basirov-m7--> </InlineEquation> mesons at high <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({{p}_{{\text{T}}}}\)</EquationSource> <!--PhysPart2570123Basirov-m8--> </InlineEquation>, azimuthal dependences of the fractional parton energy loss <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({{S}_{{{\text{loss}}}}}(\Delta \varphi )\)</EquationSource> <!--PhysPart2570123Basirov-m9--> </InlineEquation> are obtained, and dependences of the energy loss on the effective parton path length <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\({{S}_{{{\text{loss}}}}}({{L}_{{{\text{eff}}}}})\)</EquationSource> <!--PhysPart2570123Basirov-m10--> </InlineEquation> are constructed by considering the azimuthal distribution of the color charge density. Estimates of the effective medium stopping power as a function of the azimuthal angle of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\({{\pi }^{0}}\)</EquationSource> <!--PhysPart2570123Basirov-m11--> </InlineEquation>-meson emission relative to the reaction plane <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\({{\Delta E} \mathord{\left/ {\vphantom {{\Delta E} {{{L}_{{{\text{eff}}}}}(\Delta \varphi )}}} \right. \kern-0em} {{{L}_{{{\text{eff}}}}}(\Delta \varphi )}}\)</EquationSource> <!--PhysPart2570123Basirov-m12--> </InlineEquation> are also presented.</p>

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Azimuthal Dependence of the Fractional Parton Energy Loss in Cu + Au Collisions at \(\sqrt {{{s}_{{NN}}}} \) = 200 GeV

  • K. N. Basirov,
  • I. I. Borisov,
  • E. V. Bannikov,
  • Ya. A. Berdnikov

摘要

Abstract

The properties of the quark-gluon medium formed in Cu + Au collisions at an energy of \(\sqrt {{{s}_{{NN}}}} \) = 200 GeV can be investigated using information on the energy loss of high-energy partons ( \({{p}_{{\text{T}}}} \gg {{\Lambda }_{{{\text{QCD}}}}}\) ). One of the quantities that can be estimated experimentally is the fractional parton energy loss \({{S}_{{{\text{loss}}}}}\) . On the basis of the data on the elliptic flow \({{v}_{2}}\) of \({{\pi }^{0}}\) mesons at high \({{p}_{{\text{T}}}}\) , azimuthal dependences of the fractional parton energy loss \({{S}_{{{\text{loss}}}}}(\Delta \varphi )\) are obtained, and dependences of the energy loss on the effective parton path length \({{S}_{{{\text{loss}}}}}({{L}_{{{\text{eff}}}}})\) are constructed by considering the azimuthal distribution of the color charge density. Estimates of the effective medium stopping power as a function of the azimuthal angle of \({{\pi }^{0}}\) -meson emission relative to the reaction plane \({{\Delta E} \mathord{\left/ {\vphantom {{\Delta E} {{{L}_{{{\text{eff}}}}}(\Delta \varphi )}}} \right. \kern-0em} {{{L}_{{{\text{eff}}}}}(\Delta \varphi )}}\) are also presented.