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\begin{document}
  
  
  \begin{adjustbox}{center}
\begin{tabular}{ccccr}
&&& Extrapolation factor & Cross-section~(\si{\micro\barn}) \\
\midrule
 $ D^{0}$ \xspace   & $0 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2 <  y\xspace < 4.5$ & $1.0014 \pm 0.0024$  & $2709 \pm \phantom{1}2  \pm 165$\\
 $ D^{+}$ \xspace   & $0 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2 <  y\xspace < 4.5$ & $1.049 \pm 0.031$  & $1102 \pm \phantom{1}5  \pm 111$\\
\midrule
 $ D^{0}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2 <  y\xspace < 4.5$ & $1.0018 \pm 0.0025$  & $2072 \pm \phantom{1}2  \pm 124$\\
 $ D^{+}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2 <  y\xspace < 4.5$ & ---  & $834 \pm \phantom{1}2  \pm \phantom{1}78$\\
 $ D_{ s\xspace}^{+}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2 <  y\xspace < 4.5$ & ---  & $353 \pm \phantom{1}9  \pm \phantom{1}76$\\
 $ D^{*+}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2 <  y\xspace < 4.5$ & $1.102 \pm 0.081$  & $784 \pm \phantom{1}4  \pm \phantom{1}87$\\
\midrule
 $ D^{0}$ \xspace   & $0 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2.5 <  y\xspace < 4$ & ---  & $1720 \pm \phantom{1}1  \pm \phantom{1}98$\\
 $ D^{+}$ \xspace   & $0 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2.5 <  y\xspace < 4$ & ---  & $706 \pm \phantom{1}4  \pm \phantom{1}66$\\
\midrule
 $ D^{0}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2.5 <  y\xspace < 4$ & ---  & $1313 \pm \phantom{1}1  \pm \phantom{1}73$\\
 $ D^{+}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2.5 <  y\xspace < 4$ & ---  & $527 \pm \phantom{1}1  \pm\phantom{1} 45$\\
 $ D_{ s\xspace}^{+}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2.5 <  y\xspace < 4$ & ---  & $227 \pm \phantom{1}2  \pm \phantom{1}24$\\
 $ D^{*+}$ \xspace   & $1 <  p_{\mathrm{T}}\xspace < \SI{8}{\GeVc}$ & $2.5 <  y\xspace < 4$ & ---  & $493 \pm \phantom{1}2  \pm \phantom{1}41$\\
\end{tabular}
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\end{document}
