Partonic Flow and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>ϕ</mml:mi></mml:math>-Meson Production in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Au</mml:mi><mml:mo>+</mml:mo><mml:mi>Au</mml:mi></mml:math>Collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn>200</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>GeV</mml:mi></mml:math>
Аннотация
We present first measurements of the $\ensuremath{\phi}$-meson elliptic flow (${v}_{2}({p}_{T})$) and high-statistics ${p}_{T}$ distributions for different centralities from $\sqrt{{s}_{NN}}=200\text{ }\text{ }\mathrm{GeV}$ $\mathrm{Au}+\mathrm{Au}$ collisions at RHIC. In minimum bias collisions the ${v}_{2}$ of the $\ensuremath{\phi}$ meson is consistent with the trend observed for mesons. The ratio of the yields of the $\ensuremath{\Omega}$ to those of the $\ensuremath{\phi}$ as a function of transverse momentum is consistent with a model based on the recombination of thermal $s$ quarks up to ${p}_{T}\ensuremath{\sim}4\text{ }\text{ }\mathrm{GeV}/c$, but disagrees at higher momenta. The nuclear modification factor (${R}_{\mathrm{CP}}$) of $\ensuremath{\phi}$ follows the trend observed in the ${K}_{S}^{0}$ mesons rather than in $\ensuremath{\Lambda}$ baryons, supporting baryon-meson scaling. These data are consistent with $\ensuremath{\phi}$ mesons in central $\mathrm{Au}+\mathrm{Au}$ collisions being created via coalescence of thermalized $s$ quarks and the formation of a hot and dense matter with partonic collectivity at RHIC.
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