<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>ψ</mml:mi></mml:math>Production versus Transverse Momentum and Rapidity 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>
Аннотация
$J/\ensuremath{\psi}$ production 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 a rapidity range of $\ensuremath{-}2.2<y<2.2$ and a transverse momentum range of $0<{p}_{T}<9\text{ }\text{ }\mathrm{GeV}/c$. The size of the present data set allows a detailed measurement of both the ${p}_{T}$ and the rapidity distributions and is sufficient to constrain production models. The total cross section times the branching ratio is ${B}_{ll}{\ensuremath{\sigma}}_{\mathrm{pp}}^{J/\ensuremath{\psi}}=178\ifmmode\pm\else\textpm\fi{}{3}^{\mathrm{stat}}\ifmmode\pm\else\textpm\fi{}{53}^{\mathrm{sys}}\ifmmode\pm\else\textpm\fi{}{18}^{\mathrm{norm}}\text{ }\text{ }\mathrm{nb}$.
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