Measurement of High-<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>p</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:math>Single Electrons from Heavy-Flavor Decays in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mi>p</mml:mi></mml:math>Collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:mi>s</mml:mi></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>
Abstract
The momentum distribution of electrons from decays of heavy flavor (charm and bottom) for midrapidity $|y|<0.35$ in $p+p$ collisions at $\sqrt{s}=200\text{ }\text{ }\mathrm{GeV}$ has been measured by the PHENIX experiment at the BNL Relativistic Heavy Ion Collider over the transverse momentum range $0.3<{p}_{T}<9\text{ }\text{ }\mathrm{GeV}/c$. Two independent methods have been used to determine the heavy-flavor yields, and the results are in good agreement with each other. A fixed-order-plus-next-to-leading-log perturbative QCD calculation agrees with the data within the theoretical and experimental uncertainties, with the data/theory ratio of $1.71\ifmmode\pm\else\textpm\fi{}{0.02}^{\mathrm{stat}}\ifmmode\pm\else\textpm\fi{}{0.18}^{\mathrm{sys}}$ for $0.3<{p}_{T}<9\text{ }\text{ }\mathrm{GeV}/c$. The total charm production cross section at this energy has also been deduced to be ${\ensuremath{\sigma}}_{c\overline{c}}=567\ifmmode\pm\else\textpm\fi{}{57}^{\mathrm{stat}}\ifmmode\pm\else\textpm\fi{}{193}^{\mathrm{sys}}\text{ }\text{ }\ensuremath{\mu}\mathrm{b}$.
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