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Distributions of the simultaneous fits to the (left) M(Kπ+π+)M(Kπ+π+) and (right) log10\chisqiplog10\chisqip for \Dp\Dp mesons in the forward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $3.0
Distributions of the simultaneous fits to the (left) M(Kπ+π+)M(Kπ+π+) and (right) log10\chisqiplog10\chisqip for \Dp\Dp mesons in the forward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $3.0
Distributions of the simultaneous fits to the (left) M(Kπ+π+)M(Kπ+π+) and (right) log10\chisqiplog10\chisqip for \Dp\Dp mesons in the forward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $3.0
Distributions of the simultaneous fits to the (left) M(Kπ+π+)M(Kπ+π+) and (right) log10\chisqiplog10\chisqip for \Dp\Dp mesons in the forward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $3.0
Distributions of the simultaneous fits to the (left) M(Kπ+π+)M(Kπ+π+) and (right) log10\chisqiplog10\chisqip for \Dp\Dp mesons in the backward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $-4.5
Distributions of the simultaneous fits to the (left) M(Kπ+π+)M(Kπ+π+) and (right) log10\chisqiplog10\chisqip for \Dp\Dp mesons in the backward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $-4.5
Distributions of the simultaneous fits to the (left) M(KK+π+)M(KK+π+) and (right) log10\chisqiplog10\chisqip for \Ds\Ds mesons in the forward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $3.0
Distributions of the simultaneous fits to the (left) M(KK+π+)M(KK+π+) and (right) log10\chisqiplog10\chisqip for \Ds\Ds mesons in the forward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $3.0
Distributions of the simultaneous fits to the (left) M(KK+π+)M(KK+π+) and (right) log10\chisqiplog10\chisqip for \Ds\Ds mesons in the backward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $-4.5
Distributions of the simultaneous fits to the (left) M(KK+π+)M(KK+π+) and (right) log10\chisqiplog10\chisqip for \Ds\Ds mesons in the backward data sample in the kinematic bin of 2<\pt<3\gevc2<\pt<3\gevc and $-4.5
Double-differential cross-section of prompt \Dp\Dp mesons in \pPb\pPb collisions for the (left) forward and (right) backward rapidities. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty, both of which are smaller than the symbol size. The value in a particular rapidity interval is scaled by a multiplicative factor 10m10m, where the factor mm increase as the rapidity rises.
Double-differential cross-section of prompt \Dp\Dp mesons in \pPb\pPb collisions for the (left) forward and (right) backward rapidities. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty, both of which are smaller than the symbol size. The value in a particular rapidity interval is scaled by a multiplicative factor 10m10m, where the factor mm increase as the rapidity rises.
Double-differential cross-section of prompt \Dp\Dp mesons in \pPb\pPb collisions for the (left) forward and (right) backward rapidities. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty, both of which are smaller than the symbol size. The value in a particular rapidity interval is scaled by a multiplicative factor 10m10m, where the factor mm increase as the rapidity rises.
Double-differential cross-section of prompt \Dp\Dp mesons in \pPb\pPb collisions for the (left) forward and (right) backward rapidities. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty, both of which are smaller than the symbol size. The value in a particular rapidity interval is scaled by a multiplicative factor 10m10m, where the factor mm increase as the rapidity rises.
Double-differential cross-section of prompt \Ds\Ds mesons in \pPb\pPb collisions for the (left) forward and (right) backward rapidities. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty, both of which are smaller than the symbol size. The value in a particular rapidity interval is scaled by a multiplicative factor 10m10m, where the factor mm increase as the rapidity rises.
Double-differential cross-section of prompt \Ds\Ds mesons in \pPb\pPb collisions for the (left) forward and (right) backward rapidities. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty, both of which are smaller than the symbol size. The value in a particular rapidity interval is scaled by a multiplicative factor 10m10m, where the factor mm increase as the rapidity rises.
Differential cross-section of prompt \Dp\Dp meson production in \pPb\pPb collisions as a function of (left) \pt\pt and (right) yy in the forward and backward collision samples. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty.
Differential cross-section of prompt \Dp\Dp meson production in \pPb\pPb collisions as a function of (left) \pt\pt and (right) yy in the forward and backward collision samples. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty.
Differential cross-section of prompt \Dp\Dp meson production in \pPb\pPb collisions as a function of (left) \pt\pt and (right) yy in the forward and backward collision samples. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty.
Differential cross-section of prompt \Dp\Dp meson production in \pPb\pPb collisions as a function of (left) \pt\pt and (right) yy in the forward and backward collision samples. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty.
Differential cross-section of prompt \Ds\Ds meson production in \pPb\pPb collisions as a function of (left) \pt\pt and (right) yy in the forward and backward collision samples. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty.
Differential cross-section of prompt \Ds\Ds meson production in \pPb\pPb collisions as a function of (left) \pt\pt and (right) yy in the forward and backward collision samples. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty.
Nuclear modification factors R\pPbR\pPb as a function of \pt\pt for prompt \Dp\Dp and \Ds\Ds meson production in the (left) forward data and (right) backward data. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty. The CGC~\cite{Ducloue:2015gfa,Ducloue:2016ywt,Fujii:2017rqa} predictions are only available in the forward region. Previous results on \Dz mesons~\cite{LHCb:2017yua} from LHCb are also shown.
Nuclear modification factors R\pPbR\pPb as a function of \pt\pt for prompt \Dp\Dp and \Ds\Ds meson production in the (left) forward data and (right) backward data. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty. The CGC~\cite{Ducloue:2015gfa,Ducloue:2016ywt,Fujii:2017rqa} predictions are only available in the forward region. Previous results on \Dz mesons~\cite{LHCb:2017yua} from LHCb are also shown.
Nuclear modification factors R\pPbR\pPb as a function of \pt\pt for prompt \Dp\Dp and \Ds\Ds meson production in the (left) forward data and (right) backward data. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty. The CGC~\cite{Ducloue:2015gfa,Ducloue:2016ywt,Fujii:2017rqa} predictions are only available in the forward region. Previous results on \Dz mesons~\cite{LHCb:2017yua} from LHCb are also shown.
Nuclear modification factors R\pPbR\pPb as a function of \pt\pt for prompt \Dp\Dp and \Ds\Ds meson production in the (left) forward data and (right) backward data. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty. The CGC~\cite{Ducloue:2015gfa,Ducloue:2016ywt,Fujii:2017rqa} predictions are only available in the forward region. Previous results on \Dz mesons~\cite{LHCb:2017yua} from LHCb are also shown.
Nuclear modification factors R\pPbR\pPb as a function of yy for prompt \Dp\Dp and \Ds\Ds meson production, integrated up to \pt=10\gevc\pt=10\gevc. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty. The CGC~\cite{Ducloue:2015gfa,Ducloue:2016ywt,Fujii:2017rqa} predictions are only available in the forward region. Previous results on \Dz mesons~\cite{LHCb:2017yua} from LHCb are also shown.
Nuclear modification factors R\pPbR\pPb as a function of yy for prompt \Dp\Dp and \Ds\Ds meson production, integrated up to \pt=10\gevc\pt=10\gevc. The error bars are the statistical uncertainty and the boxes are the systematic uncertainty. The CGC~\cite{Ducloue:2015gfa,Ducloue:2016ywt,Fujii:2017rqa} predictions are only available in the forward region. Previous results on \Dz mesons~\cite{LHCb:2017yua} from LHCb are also shown.
Forward-backward ratios RFBRFB for prompt \Dp\Dp and \Ds\Ds meson production (left) as a function of \pt\pt; (right) as a function of yy. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty. Previous results on \Dz~\cite{LHCb:2017yua} mesons and \Lc~\cite{LHCb:2018weo} baryons from LHCb are also shown.
Forward-backward ratios RFBRFB for prompt \Dp\Dp and \Ds\Ds meson production (left) as a function of \pt\pt; (right) as a function of yy. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty. Previous results on \Dz~\cite{LHCb:2017yua} mesons and \Lc~\cite{LHCb:2018weo} baryons from LHCb are also shown.
Forward-backward ratios RFBRFB for prompt \Dp\Dp and \Ds\Ds meson production (left) as a function of \pt\pt; (right) as a function of yy. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty. Previous results on \Dz~\cite{LHCb:2017yua} mesons and \Lc~\cite{LHCb:2018weo} baryons from LHCb are also shown.
Forward-backward ratios RFBRFB for prompt \Dp\Dp and \Ds\Ds meson production (left) as a function of \pt\pt; (right) as a function of yy. The error bars are the statistical uncertainty while the boxes are the systematic uncertainty. Previous results on \Dz~\cite{LHCb:2017yua} mesons and \Lc~\cite{LHCb:2018weo} baryons from LHCb are also shown.
Production ratios as a function of \pt\pt in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with other results of pppp~\cite{LHCb:2016ikn,ALICE:2019nxm} and \pPb~\cite{Acharya:2019mno} collisions at the same centre-of-mass energy from \lhcb and ALICE.
Production ratios as a function of \pt\pt in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with other results of pppp~\cite{LHCb:2016ikn,ALICE:2019nxm} and \pPb~\cite{Acharya:2019mno} collisions at the same centre-of-mass energy from \lhcb and ALICE.
Production ratios as a function of \pt\pt in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with other results of pppp~\cite{LHCb:2016ikn,ALICE:2019nxm} and \pPb~\cite{Acharya:2019mno} collisions at the same centre-of-mass energy from \lhcb and ALICE.
Production ratios as a function of \pt\pt in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with other results of pppp~\cite{LHCb:2016ikn,ALICE:2019nxm} and \pPb~\cite{Acharya:2019mno} collisions at the same centre-of-mass energy from \lhcb and ALICE.
Production ratios as a function of \pt\pt in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with other results of pppp~\cite{LHCb:2016ikn,ALICE:2019nxm} and \pPb~\cite{Acharya:2019mno} collisions at the same centre-of-mass energy from \lhcb and ALICE.
Production ratios as a function of yy in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with the results of pppp collisions at the same centre-of-mass energy from \lhcb~\cite{LHCb:2016ikn}.
Production ratios as a function of yy in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with the results of pppp collisions at the same centre-of-mass energy from \lhcb~\cite{LHCb:2016ikn}.
Production ratios as a function of yy in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with the results of pppp collisions at the same centre-of-mass energy from \lhcb~\cite{LHCb:2016ikn}.
Production ratios as a function of yy in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with the results of pppp collisions at the same centre-of-mass energy from \lhcb~\cite{LHCb:2016ikn}.
Production ratios as a function of yy in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with the results of pppp collisions at the same centre-of-mass energy from \lhcb~\cite{LHCb:2016ikn}.
Production ratios as a function of yy in \lhcb \pPb\pPb collisions. The error bars show the statistical uncertainty while the boxes show the systematic uncertainty. The uncertainties related to the branching fractions are not shown in the figure. The measurements are also compared with the results of pppp collisions at the same centre-of-mass energy from \lhcb~\cite{LHCb:2016ikn}.