<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>892</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:msup><mml:mi/><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>resonance production in Au+Au and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:math>collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msqrt><mml:mrow><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi mathvariant="italic">NN</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msqrt><mml:mo>=</mml:mo><mml:mn>200</mml:mn><mml:mspace width="0.3em"/><mml:mi fontstyle="normal">GeV</mml:mi></mml:mrow></mml:math>
Abstract
The short-lived $K(892){}^{*}$ resonance provides an efficient tool to probe properties of the hot and dense medium produced in relativistic heavy-ion collisions. We report measurements of ${K}^{*}$ in $\sqrt{{s}_{\mathit{NN}}}=200\phantom{\rule{0.3em}{0ex}}\mathrm{GeV}$ Au+Au and $p+p$ collisions reconstructed via its hadronic decay channels $K(892){}^{*0}\ensuremath{\rightarrow}K\ensuremath{\pi}$ and $K(892){}^{*\ifmmode\pm\else\textpm\fi{}}\ensuremath{\rightarrow}{K}_{S}^{0}{\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}$ using the STAR detector at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory. The ${K}^{*0}$ mass has been studied as a function of ${p}_{T}$ in minimum bias $p+p$ and central Au+Au collisions. The ${K}^{*}\phantom{\rule{0.3em}{0ex}}{p}_{T}$ spectra for minimum bias $p+p$ interactions and for Au+Au collisions in different centralities are presented. The ${K}^{*}/K$ yield ratios for all centralities in Au+Au collisions are found to be significantly lower than the ratio in minimum bias $p+p$ collisions, indicating the importance of hadronic interactions between chemical and kinetic freeze-outs. A significant nonzero ${K}^{*0}$ elliptic flow (${v}_{2}$) is observed in Au+Au collisions and is compared to the ${K}_{S}^{0}$ and \ensuremath{\Lambda} ${v}_{2}$. The nuclear modification factor of ${K}^{*}$ at intermediate ${p}_{T}$ is similar to that of ${K}_{S}^{0}$ but different from \ensuremath{\Lambda}. This establishes a baryon-meson effect over a mass effect in the particle production at intermediate ${p}_{T}$ ($2<{p}_{T}\ensuremath{\le}4\phantom{\rule{0.3em}{0ex}}\mathrm{GeV}/c$).
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