cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.70846.v1/t9
title: "Table 9" of "Rapidity and transverse-momentum dependence of the inclusive J/$\mathbf{\psi}$ nuclear modification factor in p-Pb collisions at $\mathbf{\sqrt{\textit{s}_{NN}}}=5.02$ TeV"

description: $p_{\rm T}$-dependence of the ratio between the $R_{\rm PbPb}$ and the cold nuclear matter effects evaluated as $R_{\rm pPb}$(-4.46
description: CERN-LHC. Measurement of the rapidity and transverse-momentum dependence of the inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV at CERN LHC, in three center-of-mass rapidity ($y_{\rm cms}$) regions, down to zero $p_{\rm T}$. The measurements are performed at forward (2.03&lt;$y_{\rm cms}$&lt;3.53), mid (-1.37&lt;$y_{\rm cms}$&lt;0.43) and backward (-4.46&lt;$y_{\rm cms}$&lt;-2.96) centre of mass rapidities.
DOI: 10.17182/hepdata.70847.v1/t1
title: "Table 1" of "Pseudorapidity and transverse-momentum distributions of charged particles in proton-proton collisions at $\mathbf{\sqrt{\textit s}}$ = 13 TeV"

description: Average pseudorapidity density of charged particles as a function of eta produced in pp collisions at sqrt(s) = 13 TeV. The results are shown in the normalisation classes INEL and INEL&gt;0. The uncertainties are the quadratic sum of statistical and systematic contributions.
description: CERN-LHC. The pseudorapidity ($\eta$) and transverse-momentum ($p_{\rm T}$) distributions of charged particles produced in proton-proton collisions are measured at the centre-of-mass energy $\sqrt{s}$ = 13 TeV. The pseudorapidity distribution in $|\eta|&lt;$ 1.8 is reported for inelastic events and for events with at least one charged particle in $|\eta|&lt;$ 1. The pseudorapidity density of charged particles produced in the pseudorapidity region $|\eta|&lt;$ 0.5 is 5.31 $\pm$ 0.18 and 6.46 $\pm$ 0.19 for the two event classes, respectively. The transverse-momentum distribution of charged particles is measured in the range 0.15 $&lt;$ $p_{\rm T}$ $&lt;$ 20 GeV/c and $|\eta|&lt;$ 0.8 for events with at least one charged particle in $|\eta|&lt;$ 1 (INEL&gt;0). The correlation between transverse momentum and particle multiplicity is also investigated by studying the evolution of the spectra with event multiplicity.
DOI: 10.17182/hepdata.70847.v1/t2
title: "Table 2" of "Pseudorapidity and transverse-momentum distributions of charged particles in proton-proton collisions at $\mathbf{\sqrt{\textit s}}$ = 13 TeV"

description: Invariant charged-particle yield as a function of pT normalised to INEL&gt;0 events.
description: CERN-LHC. The pseudorapidity ($\eta$) and transverse-momentum ($p_{\rm T}$) distributions of charged particles produced in proton-proton collisions are measured at the centre-of-mass energy $\sqrt{s}$ = 13 TeV. The pseudorapidity distribution in $|\eta|&lt;$ 1.8 is reported for inelastic events and for events with at least one charged particle in $|\eta|&lt;$ 1. The pseudorapidity density of charged particles produced in the pseudorapidity region $|\eta|&lt;$ 0.5 is 5.31 $\pm$ 0.18 and 6.46 $\pm$ 0.19 for the two event classes, respectively. The transverse-momentum distribution of charged particles is measured in the range 0.15 $&lt;$ $p_{\rm T}$ $&lt;$ 20 GeV/c and $|\eta|&lt;$ 0.8 for events with at least one charged particle in $|\eta|&lt;$ 1 (INEL&gt;0). The correlation between transverse momentum and particle multiplicity is also investigated by studying the evolution of the spectra with event multiplicity.
DOI: 10.17182/hepdata.70847.v1/t3
title: "Table 3" of "Pseudorapidity and transverse-momentum distributions of charged particles in proton-proton collisions at $\mathbf{\sqrt{\textit s}}$ = 13 TeV"

description: Ratio of transverse-momentum spectra in INEL&gt;0 events at $\sqrt{s}$ = 13 and 7 TeV.
description: CERN-LHC. The pseudorapidity ($\eta$) and transverse-momentum ($p_{\rm T}$) distributions of charged particles produced in proton-proton collisions are measured at the centre-of-mass energy $\sqrt{s}$ = 13 TeV. The pseudorapidity distribution in $|\eta|&lt;$ 1.8 is reported for inelastic events and for events with at least one charged particle in $|\eta|&lt;$ 1. The pseudorapidity density of charged particles produced in the pseudorapidity region $|\eta|&lt;$ 0.5 is 5.31 $\pm$ 0.18 and 6.46 $\pm$ 0.19 for the two event classes, respectively. The transverse-momentum distribution of charged particles is measured in the range 0.15 $&lt;$ $p_{\rm T}$ $&lt;$ 20 GeV/c and $|\eta|&lt;$ 0.8 for events with at least one charged particle in $|\eta|&lt;$ 1 (INEL&gt;0). The correlation between transverse momentum and particle multiplicity is also investigated by studying the evolution of the spectra with event multiplicity.
DOI: 10.17182/hepdata.70847.v1/t4
title: "Table 4" of "Pseudorapidity and transverse-momentum distributions of charged particles in proton-proton collisions at $\mathbf{\sqrt{\textit s}}$ = 13 TeV"

description: Ratios of transverse-momentum distributions of charged particles in three intervals of multiplicities to the respective one for inclusive (INEL&gt;0) collisions. The spectra were normalised by the integral prior to division.
description: CERN-LHC. The pseudorapidity ($\eta$) and transverse-momentum ($p_{\rm T}$) distributions of charged particles produced in proton-proton collisions are measured at the centre-of-mass energy $\sqrt{s}$ = 13 TeV. The pseudorapidity distribution in $|\eta|&lt;$ 1.8 is reported for inelastic events and for events with at least one charged particle in $|\eta|&lt;$ 1. The pseudorapidity density of charged particles produced in the pseudorapidity region $|\eta|&lt;$ 0.5 is 5.31 $\pm$ 0.18 and 6.46 $\pm$ 0.19 for the two event classes, respectively. The transverse-momentum distribution of charged particles is measured in the range 0.15 $&lt;$ $p_{\rm T}$ $&lt;$ 20 GeV/c and $|\eta|&lt;$ 0.8 for events with at least one charged particle in $|\eta|&lt;$ 1 (INEL&gt;0). The correlation between transverse momentum and particle multiplicity is also investigated by studying the evolution of the spectra with event multiplicity.
DOI: 10.17182/hepdata.70861.v1/t1
title: "Table 1" of "$^{3}_{\Lambda}\mathrm H$ and $^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: (Hypertriton + Anti-Hypertriton)dN/d(ct) distribution.
description: CERN-LHC. Hypertriton and anti-hypertriton measurement in Pb--Pb collisions. Lifetime determination, transverse momentum spectra, yields and coalescence parameter were measured and compared to other identified species.
DOI: 10.17182/hepdata.70861.v1/t2
title: "Table 2" of "$^{3}_{\Lambda}\mathrm H$ and $^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Hypertriton and Anti-hypertriton $p_{\rm T}$ spectra x B.R.
description: CERN-LHC. Hypertriton and anti-hypertriton measurement in Pb--Pb collisions. Lifetime determination, transverse momentum spectra, yields and coalescence parameter were measured and compared to other identified species.
DOI: 10.17182/hepdata.70861.v1/t3
title: "Table 3" of "$^{3}_{\Lambda}\mathrm H$ and $^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: $B_2$ as a function of $p_{\rm T}$/A for Hypertriton.
description: CERN-LHC. Hypertriton and anti-hypertriton measurement in Pb--Pb collisions. Lifetime determination, transverse momentum spectra, yields and coalescence parameter were measured and compared to other identified species.
DOI: 10.17182/hepdata.70861.v1/t4
title: "Table 4" of "$^{3}_{\Lambda}\mathrm H$ and $^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Total integrated yields times the B.R. of the $^{3}_{\Lambda}H \to (^{3}{\rm He} + \pi^{-})$ decay for $^{3}_{\Lambda}H$ and $^{3}_{\overline{\Lambda}}\overline{H}$.
description: CERN-LHC. Hypertriton and anti-hypertriton measurement in Pb--Pb collisions. Lifetime determination, transverse momentum spectra, yields and coalescence parameter were measured and compared to other identified species.
DOI: 10.17182/hepdata.70866.v1/t1
title: "Table 1" of "Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector"

description: Measured fiducial cross section in the $e^+e^-e^+e^-$ channel. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
description: CERN-LHC. The ZZ production cross section in proton-proton collisions at 13 TeV center-of-mass energy is measured using $3.2~\mathrm{fb}^{-1}$ of data recorded with the ATLAS detector at the Large Hadron Collider in 2015. The considered Z boson candidates decay to an electron or muon pair of mass 66-116 GeV. The cross section is measured in a fiducial phase space reflecting the detector acceptance, defined below.

Fiducial phase space definition:
- $e^+e^-e^+e^-$ or $e^+e^-\mu^+\mu^-$ or $\mu^+\mu^-\mu^+\mu^-$
- Leptons dressed by adding four momenta of final-state photons within $\Delta R(\ell,\gamma) = 0.1$ to lepton four momentum. Only photons not originating from hadron or $\tau$ decay are included. All further requirements refer to dressed leptons
- Leptons have transverse momentum $p_T &gt; 20$ GeV
- Leptons have absolute pseudorapidity $|\eta| &lt; 2.7$
- Leptons separated by $\Delta R(\ell,\ell) &gt; 0.2$ from each other
- Form same-flavor oppositely-charged dileptons. In the case of four same-flavor leptons, form pairs in such a way that $|m_{\ell\ell,1} - m_Z| + |m_{\ell\ell,2} - m_Z|$ is minimised, where $m_{\ell\ell,1}$ ($m_{\ell\ell,2}$) is the mass of the first (second) dilepton system, and $m_Z$ is the Z boson pole mass
- Dileptons have invariant mass between 66 and 116 GeV

The measurement is inclusive with respect to hadronic activity, so any number of jets may be present in addition to the four-lepton system. Contributions from double parton scattering ($pp \rightarrow Z, Z$) are included in the measurement. For details please see the paper.

The cross section is also extrapolated to the total phase space and all Z boson decay modes. The result is model-dependent and includes phase space that was not experimentally accessible, so it should be used with caution. Whenever possible, the fiducial cross sections should be used instead, since they are only minimally model-dependent.
DOI: 10.17182/hepdata.70866.v1/t2
title: "Table 2" of "Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector"

description: Measured fiducial cross section in the $e^+e^-\mu^+\mu^-$ channel. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
description: CERN-LHC. The ZZ production cross section in proton-proton collisions at 13 TeV center-of-mass energy is measured using $3.2~\mathrm{fb}^{-1}$ of data recorded with the ATLAS detector at the Large Hadron Collider in 2015. The considered Z boson candidates decay to an electron or muon pair of mass 66-116 GeV. The cross section is measured in a fiducial phase space reflecting the detector acceptance, defined below.

Fiducial phase space definition:
- $e^+e^-e^+e^-$ or $e^+e^-\mu^+\mu^-$ or $\mu^+\mu^-\mu^+\mu^-$
- Leptons dressed by adding four momenta of final-state photons within $\Delta R(\ell,\gamma) = 0.1$ to lepton four momentum. Only photons not originating from hadron or $\tau$ decay are included. All further requirements refer to dressed leptons
- Leptons have transverse momentum $p_T &gt; 20$ GeV
- Leptons have absolute pseudorapidity $|\eta| &lt; 2.7$
- Leptons separated by $\Delta R(\ell,\ell) &gt; 0.2$ from each other
- Form same-flavor oppositely-charged dileptons. In the case of four same-flavor leptons, form pairs in such a way that $|m_{\ell\ell,1} - m_Z| + |m_{\ell\ell,2} - m_Z|$ is minimised, where $m_{\ell\ell,1}$ ($m_{\ell\ell,2}$) is the mass of the first (second) dilepton system, and $m_Z$ is the Z boson pole mass
- Dileptons have invariant mass between 66 and 116 GeV

The measurement is inclusive with respect to hadronic activity, so any number of jets may be present in addition to the four-lepton system. Contributions from double parton scattering ($pp \rightarrow Z, Z$) are included in the measurement. For details please see the paper.

The cross section is also extrapolated to the total phase space and all Z boson decay modes. The result is model-dependent and includes phase space that was not experimentally accessible, so it should be used with caution. Whenever possible, the fiducial cross sections should be used instead, since they are only minimally model-dependent.
DOI: 10.17182/hepdata.70866.v1/t3
title: "Table 3" of "Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector"

description: Measured fiducial cross section in the $\mu^+\mu^-\mu^+\mu^-$ channel. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
description: CERN-LHC. The ZZ production cross section in proton-proton collisions at 13 TeV center-of-mass energy is measured using $3.2~\mathrm{fb}^{-1}$ of data recorded with the ATLAS detector at the Large Hadron Collider in 2015. The considered Z boson candidates decay to an electron or muon pair of mass 66-116 GeV. The cross section is measured in a fiducial phase space reflecting the detector acceptance, defined below.

Fiducial phase space definition:
- $e^+e^-e^+e^-$ or $e^+e^-\mu^+\mu^-$ or $\mu^+\mu^-\mu^+\mu^-$
- Leptons dressed by adding four momenta of final-state photons within $\Delta R(\ell,\gamma) = 0.1$ to lepton four momentum. Only photons not originating from hadron or $\tau$ decay are included. All further requirements refer to dressed leptons
- Leptons have transverse momentum $p_T &gt; 20$ GeV
- Leptons have absolute pseudorapidity $|\eta| &lt; 2.7$
- Leptons separated by $\Delta R(\ell,\ell) &gt; 0.2$ from each other
- Form same-flavor oppositely-charged dileptons. In the case of four same-flavor leptons, form pairs in such a way that $|m_{\ell\ell,1} - m_Z| + |m_{\ell\ell,2} - m_Z|$ is minimised, where $m_{\ell\ell,1}$ ($m_{\ell\ell,2}$) is the mass of the first (second) dilepton system, and $m_Z$ is the Z boson pole mass
- Dileptons have invariant mass between 66 and 116 GeV

The measurement is inclusive with respect to hadronic activity, so any number of jets may be present in addition to the four-lepton system. Contributions from double parton scattering ($pp \rightarrow Z, Z$) are included in the measurement. For details please see the paper.

The cross section is also extrapolated to the total phase space and all Z boson decay modes. The result is model-dependent and includes phase space that was not experimentally accessible, so it should be used with caution. Whenever possible, the fiducial cross sections should be used instead, since they are only minimally model-dependent.
DOI: 10.17182/hepdata.70866.v1/t4
title: "Table 4" of "Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector"

description: Measured fiducial cross section in all $\ell^+\ell^-\ell'^+\ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
description: CERN-LHC. The ZZ production cross section in proton-proton collisions at 13 TeV center-of-mass energy is measured using $3.2~\mathrm{fb}^{-1}$ of data recorded with the ATLAS detector at the Large Hadron Collider in 2015. The considered Z boson candidates decay to an electron or muon pair of mass 66-116 GeV. The cross section is measured in a fiducial phase space reflecting the detector acceptance, defined below.

Fiducial phase space definition:
- $e^+e^-e^+e^-$ or $e^+e^-\mu^+\mu^-$ or $\mu^+\mu^-\mu^+\mu^-$
- Leptons dressed by adding four momenta of final-state photons within $\Delta R(\ell,\gamma) = 0.1$ to lepton four momentum. Only photons not originating from hadron or $\tau$ decay are included. All further requirements refer to dressed leptons
- Leptons have transverse momentum $p_T &gt; 20$ GeV
- Leptons have absolute pseudorapidity $|\eta| &lt; 2.7$
- Leptons separated by $\Delta R(\ell,\ell) &gt; 0.2$ from each other
- Form same-flavor oppositely-charged dileptons. In the case of four same-flavor leptons, form pairs in such a way that $|m_{\ell\ell,1} - m_Z| + |m_{\ell\ell,2} - m_Z|$ is minimised, where $m_{\ell\ell,1}$ ($m_{\ell\ell,2}$) is the mass of the first (second) dilepton system, and $m_Z$ is the Z boson pole mass
- Dileptons have invariant mass between 66 and 116 GeV

The measurement is inclusive with respect to hadronic activity, so any number of jets may be present in addition to the four-lepton system. Contributions from double parton scattering ($pp \rightarrow Z, Z$) are included in the measurement. For details please see the paper.

The cross section is also extrapolated to the total phase space and all Z boson decay modes. The result is model-dependent and includes phase space that was not experimentally accessible, so it should be used with caution. Whenever possible, the fiducial cross sections should be used instead, since they are only minimally model-dependent.
DOI: 10.17182/hepdata.70866.v1/t5
title: "Table 5" of "Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector"

description: Cross section extrapolated to total phase space and all Z boson decays. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
description: CERN-LHC. The ZZ production cross section in proton-proton collisions at 13 TeV center-of-mass energy is measured using $3.2~\mathrm{fb}^{-1}$ of data recorded with the ATLAS detector at the Large Hadron Collider in 2015. The considered Z boson candidates decay to an electron or muon pair of mass 66-116 GeV. The cross section is measured in a fiducial phase space reflecting the detector acceptance, defined below.

Fiducial phase space definition:
- $e^+e^-e^+e^-$ or $e^+e^-\mu^+\mu^-$ or $\mu^+\mu^-\mu^+\mu^-$
- Leptons dressed by adding four momenta of final-state photons within $\Delta R(\ell,\gamma) = 0.1$ to lepton four momentum. Only photons not originating from hadron or $\tau$ decay are included. All further requirements refer to dressed leptons
- Leptons have transverse momentum $p_T &gt; 20$ GeV
- Leptons have absolute pseudorapidity $|\eta| &lt; 2.7$
- Leptons separated by $\Delta R(\ell,\ell) &gt; 0.2$ from each other
- Form same-flavor oppositely-charged dileptons. In the case of four same-flavor leptons, form pairs in such a way that $|m_{\ell\ell,1} - m_Z| + |m_{\ell\ell,2} - m_Z|$ is minimised, where $m_{\ell\ell,1}$ ($m_{\ell\ell,2}$) is the mass of the first (second) dilepton system, and $m_Z$ is the Z boson pole mass
- Dileptons have invariant mass between 66 and 116 GeV

The measurement is inclusive with respect to hadronic activity, so any number of jets may be present in addition to the four-lepton system. Contributions from double parton scattering ($pp \rightarrow Z, Z$) are included in the measurement. For details please see the paper.

The cross section is also extrapolated to the total phase space and all Z boson decay modes. The result is model-dependent and includes phase space that was not experimentally accessible, so it should be used with caution. Whenever possible, the fiducial cross sections should be used instead, since they are only minimally model-dependent.
DOI: 10.17182/hepdata.70867.v1/t1
title: "Table 1" of "A Study of Inclusive Xi-, Xi (1530) and $\omega^-$ Production in $K^- p$ Interactions at 8.25-{GeV}/$c$"

description: No description provided.
description: PLAB=8.25GEV/C. B.C. DATA (SMALL PT) FROM CERN.
DOI: 10.17182/hepdata.70867.v1/t2
title: "Table 2" of "A Study of Inclusive Xi-, Xi (1530) and $\omega^-$ Production in $K^- p$ Interactions at 8.25-{GeV}/$c$"

description: No description provided.
description: PLAB=8.25GEV/C. B.C. DATA (SMALL PT) FROM CERN.
DOI: 10.17182/hepdata.70875.v1/t1
title: "Table 1" of "Inclusive Production of Multistrange Hyperons From 11-{GeV}/$c K^- p$ Interactions"

description: No description provided.
description: PLAB=11 GEV/C. DATA FROM SLAC USING THE LARGE-APERTURE SUPER- CONDUCTING SPECTROMETER.
DOI: 10.17182/hepdata.70875.v1/t2
title: "Table 2" of "Inclusive Production of Multistrange Hyperons From 11-{GeV}/$c K^- p$ Interactions"

description: No description provided.
description: PLAB=11 GEV/C. DATA FROM SLAC USING THE LARGE-APERTURE SUPER- CONDUCTING SPECTROMETER.
DOI: 10.17182/hepdata.70875.v1/t3
title: "Table 3" of "Inclusive Production of Multistrange Hyperons From 11-{GeV}/$c K^- p$ Interactions"

description: No description provided.
description: PLAB=11 GEV/C. DATA FROM SLAC USING THE LARGE-APERTURE SUPER- CONDUCTING SPECTROMETER.
DOI: 10.17182/hepdata.70879.v1/t1
title: "Table 1" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Inclusive values of the asymmetry variables.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.