cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.73526.v1/t2
title: "Table 2" of "$\rm{J}/\psi$ production at low transverse momentum in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Nuclear absorption cross section.
description: BNL-RHIC. We report on the measurement of $\rm{J}/\psi$ production in the dielectron channel at mid-rapidity (|y|&lt;1) in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the STAR experiment at the Relativistic Heavy Ion Collider. The transverse momentum $p_{T}$ spectra in p+p for $p_{T}$ &lt; 4 GeV/c and d+Au collisions for $p_{T}$ &lt; 3 GeV/c are presented. These measurements extend the STAR coverage for $\rm{J}/\psi$ production in p+p collisions to low $p_{T}$. The $$ from the measured $\rm{J}/\psi$ invariant cross section in p+p and d+Au collisions are evaluated and compared to similar measurements at other collision energies. The nuclear modification factor for $\rm{J}/\psi$ is extracted as a function of $p_{T}$ and collision centrality in d+Au and compared to model calculations using the modified nuclear Parton Distribution Function and a final-state $\rm{J}/\psi$ nuclear absorption cross section.
DOI: 10.17182/hepdata.73526.v1/t3
title: "Table 3" of "$\rm{J}/\psi$ production at low transverse momentum in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The nuclear modicifation factor vs. $p_T$ for $J\psi$ with |y| &lt; 1 in 0-100 percent central d+Au collisions.
description: BNL-RHIC. We report on the measurement of $\rm{J}/\psi$ production in the dielectron channel at mid-rapidity (|y|&lt;1) in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the STAR experiment at the Relativistic Heavy Ion Collider. The transverse momentum $p_{T}$ spectra in p+p for $p_{T}$ &lt; 4 GeV/c and d+Au collisions for $p_{T}$ &lt; 3 GeV/c are presented. These measurements extend the STAR coverage for $\rm{J}/\psi$ production in p+p collisions to low $p_{T}$. The $$ from the measured $\rm{J}/\psi$ invariant cross section in p+p and d+Au collisions are evaluated and compared to similar measurements at other collision energies. The nuclear modification factor for $\rm{J}/\psi$ is extracted as a function of $p_{T}$ and collision centrality in d+Au and compared to model calculations using the modified nuclear Parton Distribution Function and a final-state $\rm{J}/\psi$ nuclear absorption cross section.
DOI: 10.17182/hepdata.73526.v1/t4
title: "Table 4" of "$\rm{J}/\psi$ production at low transverse momentum in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Nuclear modicifation factor vs. N_coll $J\psi$ with|y|&lt;1 and pT &lt; 3 GeV/c in d Au collisions.
description: BNL-RHIC. We report on the measurement of $\rm{J}/\psi$ production in the dielectron channel at mid-rapidity (|y|&lt;1) in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the STAR experiment at the Relativistic Heavy Ion Collider. The transverse momentum $p_{T}$ spectra in p+p for $p_{T}$ &lt; 4 GeV/c and d+Au collisions for $p_{T}$ &lt; 3 GeV/c are presented. These measurements extend the STAR coverage for $\rm{J}/\psi$ production in p+p collisions to low $p_{T}$. The $$ from the measured $\rm{J}/\psi$ invariant cross section in p+p and d+Au collisions are evaluated and compared to similar measurements at other collision energies. The nuclear modification factor for $\rm{J}/\psi$ is extracted as a function of $p_{T}$ and collision centrality in d+Au and compared to model calculations using the modified nuclear Parton Distribution Function and a final-state $\rm{J}/\psi$ nuclear absorption cross section.
DOI: 10.17182/hepdata.73526.v1/t5
title: "Table 5" of "$\rm{J}/\psi$ production at low transverse momentum in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The invariant cross section versus transverse momentum for J/$\psi$ with $|y|\lt 1$ in $p+p$ collisions.
description: BNL-RHIC. We report on the measurement of $\rm{J}/\psi$ production in the dielectron channel at mid-rapidity (|y|&lt;1) in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the STAR experiment at the Relativistic Heavy Ion Collider. The transverse momentum $p_{T}$ spectra in p+p for $p_{T}$ &lt; 4 GeV/c and d+Au collisions for $p_{T}$ &lt; 3 GeV/c are presented. These measurements extend the STAR coverage for $\rm{J}/\psi$ production in p+p collisions to low $p_{T}$. The $$ from the measured $\rm{J}/\psi$ invariant cross section in p+p and d+Au collisions are evaluated and compared to similar measurements at other collision energies. The nuclear modification factor for $\rm{J}/\psi$ is extracted as a function of $p_{T}$ and collision centrality in d+Au and compared to model calculations using the modified nuclear Parton Distribution Function and a final-state $\rm{J}/\psi$ nuclear absorption cross section.
DOI: 10.17182/hepdata.73526.v1/t6
title: "Table 6" of "$\rm{J}/\psi$ production at low transverse momentum in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The invariant yield versus transverse momentum for $J/\Psi$ with |y| &lt; 1 in 0 - 100 percent central d+Au collisions.
description: BNL-RHIC. We report on the measurement of $\rm{J}/\psi$ production in the dielectron channel at mid-rapidity (|y|&lt;1) in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the STAR experiment at the Relativistic Heavy Ion Collider. The transverse momentum $p_{T}$ spectra in p+p for $p_{T}$ &lt; 4 GeV/c and d+Au collisions for $p_{T}$ &lt; 3 GeV/c are presented. These measurements extend the STAR coverage for $\rm{J}/\psi$ production in p+p collisions to low $p_{T}$. The $$ from the measured $\rm{J}/\psi$ invariant cross section in p+p and d+Au collisions are evaluated and compared to similar measurements at other collision energies. The nuclear modification factor for $\rm{J}/\psi$ is extracted as a function of $p_{T}$ and collision centrality in d+Au and compared to model calculations using the modified nuclear Parton Distribution Function and a final-state $\rm{J}/\psi$ nuclear absorption cross section.
DOI: 10.17182/hepdata.73583.v1/t1
title: "Table 1" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} p_T(\Upsilon(1S))}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t2
title: "Table 2" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} p_T(\Upsilon(1S))}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t3
title: "Table 3" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} p_T(D^0)}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t4
title: "Table 4" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} p_T(D^+)}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t5
title: "Table 5" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} y(\Upsilon(1S))}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t6
title: "Table 6" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} y(\Upsilon(1S))}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t7
title: "Table 7" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} y(D^0)}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t10
title: "Table 10" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{\pi}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} \left| \Delta \phi \right| }$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t11
title: "Table 11" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} \left| \Delta y \right| }$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t12
title: "Table 12" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} \left| \Delta y \right| }$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t13
title: "Table 13" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} p_T(\Upsilon(1S)D^0) }$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.
DOI: 10.17182/hepdata.73583.v1/t14
title: "Table 14" of "Production of associated $\Upsilon$ and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV via double parton scattering"

description: Normalized differential cross-section
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} p_T(\Upsilon(1S)D^+)}$
 for $21$ GeV/$c$.
 Only statistical uncertainties are quoted as systematic uncertainties are found to be negligible. The distribution is normalized to unity.
description: CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\sqrt{s}=7$ and $8$TeV is observed
 using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.
 The observation of five combinations, $\Upsilon(1S)D^0$, $\Upsilon(2S)D^0$, $\Upsilon(1S)D^+$, $\Upsilon(2S)D^+$
 and $\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\Upsilon(1S)D^0$ and $\Upsilon(1S)D^+$pairs
 in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton
 scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double
 parton scattering. $\Upsilon$ mesons are recontructed using $\Upsilon \to \mu^+ \mu^-$ decay mode, while for charm hadrons
 $D^0 \to K^- \pi^+$, $D^+ \to K^- \pi^+ \pi^+$, $D^+_s \to K^- K^+ \pi^+$ and $\Lambda_c \to K^- \pi^+$ decay modes are used.