cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.73583.v1/t15
title: "Table 15" 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
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} y(\Upsilon(1S)D^0) }$
 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/t8
title: "Table 8" 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
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} y(D^+)}$
 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/t9
title: "Table 9" 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
 $\frac{\pi}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} \left| \Delta \phi \right| }$
 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/t16
title: "Table 16" 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
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} y(\Upsilon(1S)D^+)}$
 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/t17
title: "Table 17" 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
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} \mathcal{A}_T }$, where $\mathcal{A}_T = \frac{p_T(\Upsilon(1S))-p_T(D^0)}{p_T(\Upsilon(1S))-p_T(D^0)}$, 
 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/t18
title: "Table 18" 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
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} \mathcal{A}_T }$, where $\mathcal{A}_T = \frac{p_T(\Upsilon(1S))-p_T(D^0)}{p_T(\Upsilon(1S))-p_T(D^0)}$,
 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/t19
title: "Table 19" 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
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^0)}{\mathrm{d} m(\Upsilon(1S)D^0) }$,
 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/t20
title: "Table 20" 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
 $\frac{1}{\sigma}\frac{ \mathrm{d}\sigma(\Upsilon(1S)D^+)}{\mathrm{d} m(\Upsilon(1S)D^+)}$
 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.
DOI: 10.17182/hepdata.73584.v1/t1
title: "Table 1" of "Search for metastable heavy charged particles with large ionization energy loss in pp collisions at $\sqrt{s} = 13$ TeV using the ATLAS experiment"

description: Mass distribution for data and expected background for stable particle searches. Also shown are two examples for signals as expected for gluino R-hadrons in the explored mass range. The uncertainty on the background estimation includes both the statistical and systematic uncertainties.
description: CERN-LHC. This paper presents a search for massive charged long-lived particles produced in pp collisions at $\sqrt{s}=$ 13 TeV at the LHC using the ATLAS experiment. The dataset used corresponds to an integrated luminosity of 3.2 fb$^{-1}$. Many extensions of the Standard Model predict the existence of massive charged long-lived particles, such as $R$-hadrons. These massive particles are expected to be produced with a velocity significantly below the speed of light, and therefore to have a specific ionization higher than any Standard Model particle of unit charge at high momenta. The Pixel subsystem of the ATLAS detector is used to measure the ionization energy loss of reconstructed charged particles and to search for such highly ionizing particles. The search presented here has much greater sensitivity than a similar search performed using the ATLAS detector in the $\sqrt{s}=$ 8 TeV dataset, thanks to the increase in expected signal cross-section due to the higher center-of-mass energy of collisions, to an upgraded detector with a new silicon layer close to the interaction point, and to analysis improvements. No significant deviation from Standard Model background expectations is observed, and lifetime-dependent upper limits on $R$-hadron production cross-sections and masses are set. Gluino $R$-hadrons with lifetimes above 0.4 ns and decaying to $q\bar{q}$ plus a 100 GeV neutralino are excluded at the 95% confidence level, with lower mass limit ranging between 740 GeV and 1590 GeV. In the case of stable $R$-hadrons the lower mass limit at the 95% confidence level is 1570 GeV.
DOI: 10.17182/hepdata.73584.v1/t2
title: "Table 2" of "Search for metastable heavy charged particles with large ionization energy loss in pp collisions at $\sqrt{s} = 13$ TeV using the ATLAS experiment"

description: Mass distribution for data and expected background for metastable particle searches. Also shown are two examples for signals as expected for gluino R-hadrons in the explored mass range. The uncertainty on the background estimation includes both the statistical and systematic uncertainties.
description: CERN-LHC. This paper presents a search for massive charged long-lived particles produced in pp collisions at $\sqrt{s}=$ 13 TeV at the LHC using the ATLAS experiment. The dataset used corresponds to an integrated luminosity of 3.2 fb$^{-1}$. Many extensions of the Standard Model predict the existence of massive charged long-lived particles, such as $R$-hadrons. These massive particles are expected to be produced with a velocity significantly below the speed of light, and therefore to have a specific ionization higher than any Standard Model particle of unit charge at high momenta. The Pixel subsystem of the ATLAS detector is used to measure the ionization energy loss of reconstructed charged particles and to search for such highly ionizing particles. The search presented here has much greater sensitivity than a similar search performed using the ATLAS detector in the $\sqrt{s}=$ 8 TeV dataset, thanks to the increase in expected signal cross-section due to the higher center-of-mass energy of collisions, to an upgraded detector with a new silicon layer close to the interaction point, and to analysis improvements. No significant deviation from Standard Model background expectations is observed, and lifetime-dependent upper limits on $R$-hadron production cross-sections and masses are set. Gluino $R$-hadrons with lifetimes above 0.4 ns and decaying to $q\bar{q}$ plus a 100 GeV neutralino are excluded at the 95% confidence level, with lower mass limit ranging between 740 GeV and 1590 GeV. In the case of stable $R$-hadrons the lower mass limit at the 95% confidence level is 1570 GeV.
DOI: 10.17182/hepdata.73584.v1/t3
title: "Table 3" of "Search for metastable heavy charged particles with large ionization energy loss in pp collisions at $\sqrt{s} = 13$ TeV using the ATLAS experiment"

description: Cross-section as a function of mass for gluino R-hadrons with lifetime tau=10 ns, decaying to qanti-q plus a light neutralino of mass=100 GeV. The central value of the observed and expected 95% upper limit on excluded cross-section is given. The 1 sigma band on the expected UL is given as an uncertainty.
description: CERN-LHC. This paper presents a search for massive charged long-lived particles produced in pp collisions at $\sqrt{s}=$ 13 TeV at the LHC using the ATLAS experiment. The dataset used corresponds to an integrated luminosity of 3.2 fb$^{-1}$. Many extensions of the Standard Model predict the existence of massive charged long-lived particles, such as $R$-hadrons. These massive particles are expected to be produced with a velocity significantly below the speed of light, and therefore to have a specific ionization higher than any Standard Model particle of unit charge at high momenta. The Pixel subsystem of the ATLAS detector is used to measure the ionization energy loss of reconstructed charged particles and to search for such highly ionizing particles. The search presented here has much greater sensitivity than a similar search performed using the ATLAS detector in the $\sqrt{s}=$ 8 TeV dataset, thanks to the increase in expected signal cross-section due to the higher center-of-mass energy of collisions, to an upgraded detector with a new silicon layer close to the interaction point, and to analysis improvements. No significant deviation from Standard Model background expectations is observed, and lifetime-dependent upper limits on $R$-hadron production cross-sections and masses are set. Gluino $R$-hadrons with lifetimes above 0.4 ns and decaying to $q\bar{q}$ plus a 100 GeV neutralino are excluded at the 95% confidence level, with lower mass limit ranging between 740 GeV and 1590 GeV. In the case of stable $R$-hadrons the lower mass limit at the 95% confidence level is 1570 GeV.
DOI: 10.17182/hepdata.73584.v1/t4
title: "Table 4" of "Search for metastable heavy charged particles with large ionization energy loss in pp collisions at $\sqrt{s} = 13$ TeV using the ATLAS experiment"

description: Excluded range of lifetimes as a function of gluino R-hadron mass. The central value of the lower-limit of the observed and expected excluded masses at the 95% CL is given.
description: CERN-LHC. This paper presents a search for massive charged long-lived particles produced in pp collisions at $\sqrt{s}=$ 13 TeV at the LHC using the ATLAS experiment. The dataset used corresponds to an integrated luminosity of 3.2 fb$^{-1}$. Many extensions of the Standard Model predict the existence of massive charged long-lived particles, such as $R$-hadrons. These massive particles are expected to be produced with a velocity significantly below the speed of light, and therefore to have a specific ionization higher than any Standard Model particle of unit charge at high momenta. The Pixel subsystem of the ATLAS detector is used to measure the ionization energy loss of reconstructed charged particles and to search for such highly ionizing particles. The search presented here has much greater sensitivity than a similar search performed using the ATLAS detector in the $\sqrt{s}=$ 8 TeV dataset, thanks to the increase in expected signal cross-section due to the higher center-of-mass energy of collisions, to an upgraded detector with a new silicon layer close to the interaction point, and to analysis improvements. No significant deviation from Standard Model background expectations is observed, and lifetime-dependent upper limits on $R$-hadron production cross-sections and masses are set. Gluino $R$-hadrons with lifetimes above 0.4 ns and decaying to $q\bar{q}$ plus a 100 GeV neutralino are excluded at the 95% confidence level, with lower mass limit ranging between 740 GeV and 1590 GeV. In the case of stable $R$-hadrons the lower mass limit at the 95% confidence level is 1570 GeV.
DOI: 10.17182/hepdata.73584.v1/t5
title: "Table 5" of "Search for metastable heavy charged particles with large ionization energy loss in pp collisions at $\sqrt{s} = 13$ TeV using the ATLAS experiment"

description: Cross-section as a function of mass for stable gluino R-hadrons. The central value of the observed and expected 95% upper limit on excluded cross-section is given. The 1 sigma band on the expected UL is given as an uncertainty.
description: CERN-LHC. This paper presents a search for massive charged long-lived particles produced in pp collisions at $\sqrt{s}=$ 13 TeV at the LHC using the ATLAS experiment. The dataset used corresponds to an integrated luminosity of 3.2 fb$^{-1}$. Many extensions of the Standard Model predict the existence of massive charged long-lived particles, such as $R$-hadrons. These massive particles are expected to be produced with a velocity significantly below the speed of light, and therefore to have a specific ionization higher than any Standard Model particle of unit charge at high momenta. The Pixel subsystem of the ATLAS detector is used to measure the ionization energy loss of reconstructed charged particles and to search for such highly ionizing particles. The search presented here has much greater sensitivity than a similar search performed using the ATLAS detector in the $\sqrt{s}=$ 8 TeV dataset, thanks to the increase in expected signal cross-section due to the higher center-of-mass energy of collisions, to an upgraded detector with a new silicon layer close to the interaction point, and to analysis improvements. No significant deviation from Standard Model background expectations is observed, and lifetime-dependent upper limits on $R$-hadron production cross-sections and masses are set. Gluino $R$-hadrons with lifetimes above 0.4 ns and decaying to $q\bar{q}$ plus a 100 GeV neutralino are excluded at the 95% confidence level, with lower mass limit ranging between 740 GeV and 1590 GeV. In the case of stable $R$-hadrons the lower mass limit at the 95% confidence level is 1570 GeV.
DOI: 10.17182/hepdata.73610.v1/t1
title: "Table 1" of "Charged-to-neutral correlation at forward rapidity in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV"

description: Multiplicity distributions of raw charged particles and photons.
description: BNL-RHIC. Event-by-event fluctuations of the ratio of inclusive charged to photon multiplicities at forward rapidity in Au+Au collision at $\sqrt{s_{NN}}$=200 GeV have been studied. Dominant contribution to such fluctuations is expected to come from correlated production of charged and neutral pions. We search for evidences of dynamical fluctuations of different physical origins. Observables constructed out of moments of multiplicities are used as measures of fluctuations. Mixed events and model calculations are used as baselines. Results are compared to the dynamical net-charge fluctuations measured in the same acceptance. A non-zero statistically significant signal of dynamical fluctuations is observed in excess to the model prediction when charged particles and photons are measured in the same acceptance. We find that, unlike dynamical net-charge fluctuation, charge-neutral fluctuation is not dominated by correlation due to particle decay. Results are compared to the expectations based on the generic production mechanism of pions due to isospin symmetry, for which no significant (\langle 1%) deviation is observed.