cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.73056.v1/t2
title: "Table 2" of "Search for pair-produced vector-like B quarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Event yields for the muon + jets categories.
description: CERN-LHC. A search for the production of a heavy B quark, having electric charge -1/3 and vector couplings to W, Z, and H bosons, is carried out using proton-proton collision data recorded at the CERN LHC by the CMS experiment, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The B quark is assumed to be pair-produced and to decay in one of three ways: to tW, bZ, or bH. The search is carried out in final states with one, two, and more than two charged leptons, as well as in fully hadronic final states. Each of the channels in the exclusive final-state topologies is designed to be sensitive to specific combinations of the B quark-antiquark pair decays. The observed event yields are found to be consistent with the standard model expectations in all the final states studied. A statistical combination of these results is performed and upper limits are set on the cross section of the strongly produced B quark-antiquark pairs as a function of the B quark mass. Lower limits on the B quark mass between 740 and 900 GeV are set at a 95% confidence level, depending on the values of the branching fractions of the B quark to tW, bZ, and bH. Overall, these limits are the most stringent to date.
DOI: 10.17182/hepdata.73056.v1/t3
title: "Table 3" of "Search for pair-produced vector-like B quarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Event yields for the same-sign dilepton e+e category.
description: CERN-LHC. A search for the production of a heavy B quark, having electric charge -1/3 and vector couplings to W, Z, and H bosons, is carried out using proton-proton collision data recorded at the CERN LHC by the CMS experiment, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The B quark is assumed to be pair-produced and to decay in one of three ways: to tW, bZ, or bH. The search is carried out in final states with one, two, and more than two charged leptons, as well as in fully hadronic final states. Each of the channels in the exclusive final-state topologies is designed to be sensitive to specific combinations of the B quark-antiquark pair decays. The observed event yields are found to be consistent with the standard model expectations in all the final states studied. A statistical combination of these results is performed and upper limits are set on the cross section of the strongly produced B quark-antiquark pairs as a function of the B quark mass. Lower limits on the B quark mass between 740 and 900 GeV are set at a 95% confidence level, depending on the values of the branching fractions of the B quark to tW, bZ, and bH. Overall, these limits are the most stringent to date.
DOI: 10.17182/hepdata.73056.v1/t4
title: "Table 4" of "Search for pair-produced vector-like B quarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Event yields for the same-sign dilepton mu+mu category.
description: CERN-LHC. A search for the production of a heavy B quark, having electric charge -1/3 and vector couplings to W, Z, and H bosons, is carried out using proton-proton collision data recorded at the CERN LHC by the CMS experiment, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The B quark is assumed to be pair-produced and to decay in one of three ways: to tW, bZ, or bH. The search is carried out in final states with one, two, and more than two charged leptons, as well as in fully hadronic final states. Each of the channels in the exclusive final-state topologies is designed to be sensitive to specific combinations of the B quark-antiquark pair decays. The observed event yields are found to be consistent with the standard model expectations in all the final states studied. A statistical combination of these results is performed and upper limits are set on the cross section of the strongly produced B quark-antiquark pairs as a function of the B quark mass. Lower limits on the B quark mass between 740 and 900 GeV are set at a 95% confidence level, depending on the values of the branching fractions of the B quark to tW, bZ, and bH. Overall, these limits are the most stringent to date.
DOI: 10.17182/hepdata.73056.v1/t5
title: "Table 5" of "Search for pair-produced vector-like B quarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Event yields for the same-sign dilepton mu+e category.
description: CERN-LHC. A search for the production of a heavy B quark, having electric charge -1/3 and vector couplings to W, Z, and H bosons, is carried out using proton-proton collision data recorded at the CERN LHC by the CMS experiment, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The B quark is assumed to be pair-produced and to decay in one of three ways: to tW, bZ, or bH. The search is carried out in final states with one, two, and more than two charged leptons, as well as in fully hadronic final states. Each of the channels in the exclusive final-state topologies is designed to be sensitive to specific combinations of the B quark-antiquark pair decays. The observed event yields are found to be consistent with the standard model expectations in all the final states studied. A statistical combination of these results is performed and upper limits are set on the cross section of the strongly produced B quark-antiquark pairs as a function of the B quark mass. Lower limits on the B quark mass between 740 and 900 GeV are set at a 95% confidence level, depending on the values of the branching fractions of the B quark to tW, bZ, and bH. Overall, these limits are the most stringent to date.
DOI: 10.17182/hepdata.73056.v1/t7
title: "Table 7" of "Search for pair-produced vector-like B quarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Event yields for the all-hadronic event categories.
description: CERN-LHC. A search for the production of a heavy B quark, having electric charge -1/3 and vector couplings to W, Z, and H bosons, is carried out using proton-proton collision data recorded at the CERN LHC by the CMS experiment, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The B quark is assumed to be pair-produced and to decay in one of three ways: to tW, bZ, or bH. The search is carried out in final states with one, two, and more than two charged leptons, as well as in fully hadronic final states. Each of the channels in the exclusive final-state topologies is designed to be sensitive to specific combinations of the B quark-antiquark pair decays. The observed event yields are found to be consistent with the standard model expectations in all the final states studied. A statistical combination of these results is performed and upper limits are set on the cross section of the strongly produced B quark-antiquark pairs as a function of the B quark mass. Lower limits on the B quark mass between 740 and 900 GeV are set at a 95% confidence level, depending on the values of the branching fractions of the B quark to tW, bZ, and bH. Overall, these limits are the most stringent to date.
DOI: 10.17182/hepdata.73056.v1/t8
title: "Table 8" of "Search for pair-produced vector-like B quarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Event yields for the opposite sign dilepton event categories.
description: CERN-LHC. A search for the production of a heavy B quark, having electric charge -1/3 and vector couplings to W, Z, and H bosons, is carried out using proton-proton collision data recorded at the CERN LHC by the CMS experiment, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The B quark is assumed to be pair-produced and to decay in one of three ways: to tW, bZ, or bH. The search is carried out in final states with one, two, and more than two charged leptons, as well as in fully hadronic final states. Each of the channels in the exclusive final-state topologies is designed to be sensitive to specific combinations of the B quark-antiquark pair decays. The observed event yields are found to be consistent with the standard model expectations in all the final states studied. A statistical combination of these results is performed and upper limits are set on the cross section of the strongly produced B quark-antiquark pairs as a function of the B quark mass. Lower limits on the B quark mass between 740 and 900 GeV are set at a 95% confidence level, depending on the values of the branching fractions of the B quark to tW, bZ, and bH. Overall, these limits are the most stringent to date.
DOI: 10.17182/hepdata.73056.v1/t9
title: "Table 9" of "Search for pair-produced vector-like B quarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: Cross section limits for all branching ratio combinations.
description: CERN-LHC. A search for the production of a heavy B quark, having electric charge -1/3 and vector couplings to W, Z, and H bosons, is carried out using proton-proton collision data recorded at the CERN LHC by the CMS experiment, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The B quark is assumed to be pair-produced and to decay in one of three ways: to tW, bZ, or bH. The search is carried out in final states with one, two, and more than two charged leptons, as well as in fully hadronic final states. Each of the channels in the exclusive final-state topologies is designed to be sensitive to specific combinations of the B quark-antiquark pair decays. The observed event yields are found to be consistent with the standard model expectations in all the final states studied. A statistical combination of these results is performed and upper limits are set on the cross section of the strongly produced B quark-antiquark pairs as a function of the B quark mass. Lower limits on the B quark mass between 740 and 900 GeV are set at a 95% confidence level, depending on the values of the branching fractions of the B quark to tW, bZ, and bH. Overall, these limits are the most stringent to date.
DOI: 10.17182/hepdata.73066.v1/t1
title: "Table 1" of "Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$"

description: Differential production cross-sections for prompt $D^{0} + \bar{D}^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.
description: CERN-LHC. Production cross-sections of prompt charm mesons are measured with the first data from $pp$ collisions at the LHC at a centre-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of $4.98 \pm 0.19$ pb$^{-1}$ collected by the LHCb experiment. The production cross-sections of $D^{0}$, $D^{+}$, $D_{s}^{+}$, and $D^{*+}$ mesons are measured in bins of charm meson transverse momentum, $p_{\mathrm{T}}$, and rapidity, $y$, and cover the range $0 &lt; p_{\mathrm{T}} &lt; 15$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$. The inclusive cross-sections for the four mesons, including charge conjugation, and $c\bar{c}$ within the range of $1 &lt; p_{\mathrm{T}} &lt; 8$ GeV/$c$ are found to be
\begin{equation*} 
\sigma(pp \to D^{0} X) = 2470 \pm \phantom{1}3 \pm 130\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{+} X) = 1000 \pm \phantom{1}3 \pm 110\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D_{s}^{+} X) = 460 \pm 13 \pm 100\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{*+} X) = 880 \pm \phantom{1}5 \pm 140\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to c\bar{c} X) = 2840 \pm \phantom{1}3 \pm 170 \pm 150 \,\mu\mathrm{b}
\end{equation*}
where the first uncertainty is statistical, the second is systematic and the third one, for $c\bar{c}$ only, is the fragmentation fraction uncertainty.
UPDATE (20 Sep 2016): Modified Tables 1, 5, 9, 10 and 11, updated attached correlation matrices and the inclusive $D^{0}$ and $c\bar{c}$ cross-section values according to Erratum JHEP 1609 (2016) 013.
DOI: 10.17182/hepdata.73066.v1/t2
title: "Table 2" of "Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$"

description: Differential production cross-sections for prompt $D^{+} + D^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.
description: CERN-LHC. Production cross-sections of prompt charm mesons are measured with the first data from $pp$ collisions at the LHC at a centre-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of $4.98 \pm 0.19$ pb$^{-1}$ collected by the LHCb experiment. The production cross-sections of $D^{0}$, $D^{+}$, $D_{s}^{+}$, and $D^{*+}$ mesons are measured in bins of charm meson transverse momentum, $p_{\mathrm{T}}$, and rapidity, $y$, and cover the range $0 &lt; p_{\mathrm{T}} &lt; 15$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$. The inclusive cross-sections for the four mesons, including charge conjugation, and $c\bar{c}$ within the range of $1 &lt; p_{\mathrm{T}} &lt; 8$ GeV/$c$ are found to be
\begin{equation*} 
\sigma(pp \to D^{0} X) = 2470 \pm \phantom{1}3 \pm 130\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{+} X) = 1000 \pm \phantom{1}3 \pm 110\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D_{s}^{+} X) = 460 \pm 13 \pm 100\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{*+} X) = 880 \pm \phantom{1}5 \pm 140\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to c\bar{c} X) = 2840 \pm \phantom{1}3 \pm 170 \pm 150 \,\mu\mathrm{b}
\end{equation*}
where the first uncertainty is statistical, the second is systematic and the third one, for $c\bar{c}$ only, is the fragmentation fraction uncertainty.
UPDATE (20 Sep 2016): Modified Tables 1, 5, 9, 10 and 11, updated attached correlation matrices and the inclusive $D^{0}$ and $c\bar{c}$ cross-section values according to Erratum JHEP 1609 (2016) 013.
DOI: 10.17182/hepdata.73066.v1/t3
title: "Table 3" of "Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$"

description: Differential production cross-sections for prompt $D_{s}^{+} + D_{s}^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.
description: CERN-LHC. Production cross-sections of prompt charm mesons are measured with the first data from $pp$ collisions at the LHC at a centre-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of $4.98 \pm 0.19$ pb$^{-1}$ collected by the LHCb experiment. The production cross-sections of $D^{0}$, $D^{+}$, $D_{s}^{+}$, and $D^{*+}$ mesons are measured in bins of charm meson transverse momentum, $p_{\mathrm{T}}$, and rapidity, $y$, and cover the range $0 &lt; p_{\mathrm{T}} &lt; 15$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$. The inclusive cross-sections for the four mesons, including charge conjugation, and $c\bar{c}$ within the range of $1 &lt; p_{\mathrm{T}} &lt; 8$ GeV/$c$ are found to be
\begin{equation*} 
\sigma(pp \to D^{0} X) = 2470 \pm \phantom{1}3 \pm 130\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{+} X) = 1000 \pm \phantom{1}3 \pm 110\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D_{s}^{+} X) = 460 \pm 13 \pm 100\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{*+} X) = 880 \pm \phantom{1}5 \pm 140\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to c\bar{c} X) = 2840 \pm \phantom{1}3 \pm 170 \pm 150 \,\mu\mathrm{b}
\end{equation*}
where the first uncertainty is statistical, the second is systematic and the third one, for $c\bar{c}$ only, is the fragmentation fraction uncertainty.
UPDATE (20 Sep 2016): Modified Tables 1, 5, 9, 10 and 11, updated attached correlation matrices and the inclusive $D^{0}$ and $c\bar{c}$ cross-section values according to Erratum JHEP 1609 (2016) 013.
DOI: 10.17182/hepdata.73066.v1/t4
title: "Table 4" of "Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$"

description: Differential production cross-sections in for prompt $D^{*+} + D^{*-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.
description: CERN-LHC. Production cross-sections of prompt charm mesons are measured with the first data from $pp$ collisions at the LHC at a centre-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of $4.98 \pm 0.19$ pb$^{-1}$ collected by the LHCb experiment. The production cross-sections of $D^{0}$, $D^{+}$, $D_{s}^{+}$, and $D^{*+}$ mesons are measured in bins of charm meson transverse momentum, $p_{\mathrm{T}}$, and rapidity, $y$, and cover the range $0 &lt; p_{\mathrm{T}} &lt; 15$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$. The inclusive cross-sections for the four mesons, including charge conjugation, and $c\bar{c}$ within the range of $1 &lt; p_{\mathrm{T}} &lt; 8$ GeV/$c$ are found to be
\begin{equation*} 
\sigma(pp \to D^{0} X) = 2470 \pm \phantom{1}3 \pm 130\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{+} X) = 1000 \pm \phantom{1}3 \pm 110\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D_{s}^{+} X) = 460 \pm 13 \pm 100\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{*+} X) = 880 \pm \phantom{1}5 \pm 140\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to c\bar{c} X) = 2840 \pm \phantom{1}3 \pm 170 \pm 150 \,\mu\mathrm{b}
\end{equation*}
where the first uncertainty is statistical, the second is systematic and the third one, for $c\bar{c}$ only, is the fragmentation fraction uncertainty.
UPDATE (20 Sep 2016): Modified Tables 1, 5, 9, 10 and 11, updated attached correlation matrices and the inclusive $D^{0}$ and $c\bar{c}$ cross-section values according to Erratum JHEP 1609 (2016) 013.
DOI: 10.17182/hepdata.73066.v1/t5
title: "Table 5" of "Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$"

description: The ratios of differential production cross-sections, $R_{13/7}$, for prompt $D^{0} + \bar{D}^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.
description: CERN-LHC. Production cross-sections of prompt charm mesons are measured with the first data from $pp$ collisions at the LHC at a centre-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of $4.98 \pm 0.19$ pb$^{-1}$ collected by the LHCb experiment. The production cross-sections of $D^{0}$, $D^{+}$, $D_{s}^{+}$, and $D^{*+}$ mesons are measured in bins of charm meson transverse momentum, $p_{\mathrm{T}}$, and rapidity, $y$, and cover the range $0 &lt; p_{\mathrm{T}} &lt; 15$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$. The inclusive cross-sections for the four mesons, including charge conjugation, and $c\bar{c}$ within the range of $1 &lt; p_{\mathrm{T}} &lt; 8$ GeV/$c$ are found to be
\begin{equation*} 
\sigma(pp \to D^{0} X) = 2470 \pm \phantom{1}3 \pm 130\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{+} X) = 1000 \pm \phantom{1}3 \pm 110\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D_{s}^{+} X) = 460 \pm 13 \pm 100\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{*+} X) = 880 \pm \phantom{1}5 \pm 140\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to c\bar{c} X) = 2840 \pm \phantom{1}3 \pm 170 \pm 150 \,\mu\mathrm{b}
\end{equation*}
where the first uncertainty is statistical, the second is systematic and the third one, for $c\bar{c}$ only, is the fragmentation fraction uncertainty.
UPDATE (20 Sep 2016): Modified Tables 1, 5, 9, 10 and 11, updated attached correlation matrices and the inclusive $D^{0}$ and $c\bar{c}$ cross-section values according to Erratum JHEP 1609 (2016) 013.
DOI: 10.17182/hepdata.73066.v1/t6
title: "Table 6" of "Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$"

description: The ratios of differential production cross-sections, $R_{13/7}$, for prompt $D^{+} + D^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.
description: CERN-LHC. Production cross-sections of prompt charm mesons are measured with the first data from $pp$ collisions at the LHC at a centre-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of $4.98 \pm 0.19$ pb$^{-1}$ collected by the LHCb experiment. The production cross-sections of $D^{0}$, $D^{+}$, $D_{s}^{+}$, and $D^{*+}$ mesons are measured in bins of charm meson transverse momentum, $p_{\mathrm{T}}$, and rapidity, $y$, and cover the range $0 &lt; p_{\mathrm{T}} &lt; 15$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$. The inclusive cross-sections for the four mesons, including charge conjugation, and $c\bar{c}$ within the range of $1 &lt; p_{\mathrm{T}} &lt; 8$ GeV/$c$ are found to be
\begin{equation*} 
\sigma(pp \to D^{0} X) = 2470 \pm \phantom{1}3 \pm 130\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{+} X) = 1000 \pm \phantom{1}3 \pm 110\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D_{s}^{+} X) = 460 \pm 13 \pm 100\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{*+} X) = 880 \pm \phantom{1}5 \pm 140\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to c\bar{c} X) = 2840 \pm \phantom{1}3 \pm 170 \pm 150 \,\mu\mathrm{b}
\end{equation*}
where the first uncertainty is statistical, the second is systematic and the third one, for $c\bar{c}$ only, is the fragmentation fraction uncertainty.
UPDATE (20 Sep 2016): Modified Tables 1, 5, 9, 10 and 11, updated attached correlation matrices and the inclusive $D^{0}$ and $c\bar{c}$ cross-section values according to Erratum JHEP 1609 (2016) 013.
DOI: 10.17182/hepdata.73066.v1/t7
title: "Table 7" of "Measurements of prompt charm production cross-sections in $pp$ collisions at $\sqrt{s} = 13\,\mathrm{TeV}$"

description: The ratios of differential production cross-sections, $R_{13/7}$, for prompt $D_{s}^{+} + D_{s}^{+}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.
description: CERN-LHC. Production cross-sections of prompt charm mesons are measured with the first data from $pp$ collisions at the LHC at a centre-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of $4.98 \pm 0.19$ pb$^{-1}$ collected by the LHCb experiment. The production cross-sections of $D^{0}$, $D^{+}$, $D_{s}^{+}$, and $D^{*+}$ mesons are measured in bins of charm meson transverse momentum, $p_{\mathrm{T}}$, and rapidity, $y$, and cover the range $0 &lt; p_{\mathrm{T}} &lt; 15$ GeV/$c$ and $2.0 &lt; y &lt; 4.5$. The inclusive cross-sections for the four mesons, including charge conjugation, and $c\bar{c}$ within the range of $1 &lt; p_{\mathrm{T}} &lt; 8$ GeV/$c$ are found to be
\begin{equation*} 
\sigma(pp \to D^{0} X) = 2470 \pm \phantom{1}3 \pm 130\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{+} X) = 1000 \pm \phantom{1}3 \pm 110\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D_{s}^{+} X) = 460 \pm 13 \pm 100\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to D^{*+} X) = 880 \pm \phantom{1}5 \pm 140\,\mu\mathrm{b}
\end{equation*}
\begin{equation*} 
\sigma(pp \to c\bar{c} X) = 2840 \pm \phantom{1}3 \pm 170 \pm 150 \,\mu\mathrm{b}
\end{equation*}
where the first uncertainty is statistical, the second is systematic and the third one, for $c\bar{c}$ only, is the fragmentation fraction uncertainty.
UPDATE (20 Sep 2016): Modified Tables 1, 5, 9, 10 and 11, updated attached correlation matrices and the inclusive $D^{0}$ and $c\bar{c}$ cross-section values according to Erratum JHEP 1609 (2016) 013.