cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77048.v1/t1
title: "Table 1" of "Study of $D^{+} \to K^{-} \pi^+ e^+ \nu_e$"

description: The $S$-wave phase $\delta_{S}$ measured in the 12 $m_{K\pi}$ bins with statistical and systematic uncertainties. The systematic uncertainties include: (I) background fraction, (II) background shape, (III) the $\bar K_{0}^{*}(1430)^{0}$ mass and width, (IV) additional resonances, (V) tracking efficiency correction, (VI) PID efficiency correction.
description: BEPC-BES. We present an analysis of the decay $D^{+} \to K^{-} \pi^+ e^+ \nu_e$ based on data collected by the BESIII experiment at the $\psi(3770)$ resonance. Using a nearly background-free sample of 18262 events, we measure the branching fraction $\mathcal{B}(D^{+} \to K^{-} \pi^+ e^+ \nu_e) = (3.77 \pm 0.03 \pm 0.08)\%$. For $0.8
DOI: 10.17182/hepdata.77048.v1/t2
title: "Table 2" of "Study of $D^{+} \to K^{-} \pi^+ e^+ \nu_e$"

description: Average form-factor products in the $K^{*}$-dominated region.
description: BEPC-BES. We present an analysis of the decay $D^{+} \to K^{-} \pi^+ e^+ \nu_e$ based on data collected by the BESIII experiment at the $\psi(3770)$ resonance. Using a nearly background-free sample of 18262 events, we measure the branching fraction $\mathcal{B}(D^{+} \to K^{-} \pi^+ e^+ \nu_e) = (3.77 \pm 0.03 \pm 0.08)\%$. For $0.8
DOI: 10.17182/hepdata.77051.v1/t1
title: "Table 1" of "Measurement of the Multiple-Muon Charge Ratio in the MINOS Far Detector"

description: Efficiency-corrected charge ratios as a function of measured muon multiplicity, $M$.
description: Numbers taken from table 6 of arXiv:1602.00783v4.
DOI: 10.17182/hepdata.77052.v1/t1
title: "Table 1" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Total signal cross-section per nucleon integrated over all the muon kinematics phase space in Analysis I.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t2
title: "Table 2" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Results of the double differential cross-section measurement bin-by-bin in Analysis I.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t3
title: "Table 3" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Covariance matrix for shape systematics error in Analysis I.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t4
title: "Table 4" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Covariance matrix for statistical errors in Analysis I.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t10
title: "Table 10" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Covariance matrix for flux normalization error (fully correlated) in Analysis II.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t5
title: "Table 5" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Covariance matrix for flux normalization error (fully correlated) in Analysis I.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t6
title: "Table 6" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Total signal cross-section per nucleon integrated over the restricted muon kinematics phase space ($p_\mu &gt; 0.2$ GeV and $\cos\theta_\mu &gt; 0.6$) in Analysis II.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t7
title: "Table 7" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Results of the double differential cross-section measurement bin-by-bin in Analysis II.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t9
title: "Table 9" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Covariance matrix for statistical errors in Analysis II.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77052.v1/t8
title: "Table 8" of "Measurement of double-differential muon neutrino charged-current interactions on C$_8$H$_8$ without pions in the final state using the T2K off-axis beam"

description: Covariance matrix for shape systematics error in Analysis II.
description: Numbers taken from http://t2k-experiment.org/wp-content/uploads/nd280data-numu-cc0pi-xs-on-c-2015.tar. Cross-section results as a function of muon momentum for different muon angular ranges. To get the total error you need to sum the three covariance matrices. The binning of the covariance matrices starts with the first momentum bin of the first $\cos\theta_\mu$ range and it loops over all the momentum bins of that range then it moves to the second angular range and so on.
DOI: 10.17182/hepdata.77053.v1/t1
title: "Table 1" of "Study of $\psi$ decays to the $\Xi^{-}\bar\Xi^{+}$ and $\Sigma(1385)^{\mp}\bar\Sigma(1385)^{\pm}$ final states"

description: The number of the observed events $N_\rm{obs.}$, efficiencies $\epsilon$, $\alpha$ values, and branching fractions ${\cal B}$ for $\psi\rightarrow\Xi^{-}\bar\Xi^{+}$, $\Sigma(1385)^{\mp}\bar\Sigma(1385)^{\pm}$. Only statistical uncertainties are indicated.
description: Numbers taken from table 1 of arXiv:1602.06754v3.
DOI: 10.17182/hepdata.77054.v1/t1
title: "Table 1" of "Measurement of the forward-backward asymmetry of top-quark and antiquark pairs using the full CDF Run II data set"

description: Bin centroids and the differential $A_{\rm{FB}}^{t\bar{t}}$ in the $A_{\rm{FB}}^{t\bar{t}}$ vs. $|\Delta y|$ measurement in the lepton+jets final state.
description: Numbers taken from Tables 5 and 6 of arXiv:1602.09015v1.
DOI: 10.17182/hepdata.77054.v1/t2
title: "Table 2" of "Measurement of the forward-backward asymmetry of top-quark and antiquark pairs using the full CDF Run II data set"

description: Bin centroids and the differential $A_{\rm{FB}}^{t\bar{t}}$ in the $A_{\rm{FB}}^{t\bar{t}}$ vs. $|\Delta y|$ measurement in the dilepton final state.
description: Numbers taken from Tables 5 and 6 of arXiv:1602.09015v1.
DOI: 10.17182/hepdata.77054.v1/t3
title: "Table 3" of "Measurement of the forward-backward asymmetry of top-quark and antiquark pairs using the full CDF Run II data set"

description: The eigenvalues and eigenvectors for the $A_{\rm{FB}}^{t\bar{t}}$ vs. $|\Delta y|$ measurements in both the lepton+jets and the dilepton final states. Each row contains first an eigenvalue, then the error eigenvector that corresponds to that eigenvalue.
description: Numbers taken from Tables 5 and 6 of arXiv:1602.09015v1.
DOI: 10.17182/hepdata.77057.v1/t1
title: "Table 1" of "$\phi$-meson production at forward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV and in pp collisions at $\sqrt{s}$ = 2.76 TeV"

description: $p_{\rm T}$-differential production cross section of $\phi$ in pp at $\sqrt{s_{\rm NN}}$=2.76 TeV, 
in the rapidity range 2.5 &lt; y &lt; 4
description: CERN-LHC. The first measurement of $\phi$-meson production in p-Pb collisions at a nucleon-nucleon centre-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV has been performed with the ALICE apparatus at the LHC. $\phi$-mesons have been identified in the dimuon decay channel in the transverse momentum ($p_{\rm T}$) range $1 &lt; p_{\rm T} &lt; 7$ GeV/$c$, both in the p-going ($2.03 &lt; y &lt; 3.53$) and the Pb-going ($-4.46 &lt; y &lt; -2.96$) directions, where $y$ stands for the rapidity in the nucleon-nucleon centre-of-mass. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward asymmetry for phi-meson production is measured for $2.96&lt;|y|&lt;3.53$, showing no significant $p_{\rm T}$ dependence within the uncertainties. The $p_{\rm T}$-dependence of the phi nuclear modification factor $R_{\rm pPb}$ exhibits an enhancement up to a factor 1.6 at $p_{\rm T}$ = 3-4 GeV/$c$ in the Pb-going direction. The $p_{\rm T}$-dependence of the $\phi$-meson cross section in pp collisions at $\sqrt{s}$ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for $1 &lt; p_{\rm T} &lt; 5$ GeV/$c$ and $2.5
DOI: 10.17182/hepdata.77057.v1/t2
title: "Table 2" of "$\phi$-meson production at forward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV and in pp collisions at $\sqrt{s}$ = 2.76 TeV"

description: $p_{\rm T}$-differential production cross section of $\phi$ in p-Pb at $\sqrt{s_{\rm NN}}$=5.02 TeV, 
in the rapidity range 4.46 &lt; y &lt; 2.96
description: CERN-LHC. The first measurement of $\phi$-meson production in p-Pb collisions at a nucleon-nucleon centre-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV has been performed with the ALICE apparatus at the LHC. $\phi$-mesons have been identified in the dimuon decay channel in the transverse momentum ($p_{\rm T}$) range $1 &lt; p_{\rm T} &lt; 7$ GeV/$c$, both in the p-going ($2.03 &lt; y &lt; 3.53$) and the Pb-going ($-4.46 &lt; y &lt; -2.96$) directions, where $y$ stands for the rapidity in the nucleon-nucleon centre-of-mass. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward asymmetry for phi-meson production is measured for $2.96&lt;|y|&lt;3.53$, showing no significant $p_{\rm T}$ dependence within the uncertainties. The $p_{\rm T}$-dependence of the phi nuclear modification factor $R_{\rm pPb}$ exhibits an enhancement up to a factor 1.6 at $p_{\rm T}$ = 3-4 GeV/$c$ in the Pb-going direction. The $p_{\rm T}$-dependence of the $\phi$-meson cross section in pp collisions at $\sqrt{s}$ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for $1 &lt; p_{\rm T} &lt; 5$ GeV/$c$ and $2.5
DOI: 10.17182/hepdata.77057.v1/t3
title: "Table 3" of "$\phi$-meson production at forward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV and in pp collisions at $\sqrt{s}$ = 2.76 TeV"

description: $p_{\rm T}$-differential production cross section of $\phi$ in p-Pb at $\sqrt{s_{\rm NN}}$=5.02 TeV, 
in the rapidity range 2.03 &lt; y &lt; 3.53
description: CERN-LHC. The first measurement of $\phi$-meson production in p-Pb collisions at a nucleon-nucleon centre-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV has been performed with the ALICE apparatus at the LHC. $\phi$-mesons have been identified in the dimuon decay channel in the transverse momentum ($p_{\rm T}$) range $1 &lt; p_{\rm T} &lt; 7$ GeV/$c$, both in the p-going ($2.03 &lt; y &lt; 3.53$) and the Pb-going ($-4.46 &lt; y &lt; -2.96$) directions, where $y$ stands for the rapidity in the nucleon-nucleon centre-of-mass. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward asymmetry for phi-meson production is measured for $2.96&lt;|y|&lt;3.53$, showing no significant $p_{\rm T}$ dependence within the uncertainties. The $p_{\rm T}$-dependence of the phi nuclear modification factor $R_{\rm pPb}$ exhibits an enhancement up to a factor 1.6 at $p_{\rm T}$ = 3-4 GeV/$c$ in the Pb-going direction. The $p_{\rm T}$-dependence of the $\phi$-meson cross section in pp collisions at $\sqrt{s}$ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for $1 &lt; p_{\rm T} &lt; 5$ GeV/$c$ and $2.5
DOI: 10.17182/hepdata.77057.v1/t4
title: "Table 4" of "$\phi$-meson production at forward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV and in pp collisions at $\sqrt{s}$ = 2.76 TeV"

description: $y$-differential production cross section of $\phi$ in p-Pb at $\sqrt{s_{\rm NN}}$=5.02 TeV, 
in $p_{\rm T}$ range 2.03 &lt; $p_{\rm T}$ &lt; 3.53
description: CERN-LHC. The first measurement of $\phi$-meson production in p-Pb collisions at a nucleon-nucleon centre-of-mass energy $\sqrt{s_{\rm NN}}$ = 5.02 TeV has been performed with the ALICE apparatus at the LHC. $\phi$-mesons have been identified in the dimuon decay channel in the transverse momentum ($p_{\rm T}$) range $1 &lt; p_{\rm T} &lt; 7$ GeV/$c$, both in the p-going ($2.03 &lt; y &lt; 3.53$) and the Pb-going ($-4.46 &lt; y &lt; -2.96$) directions, where $y$ stands for the rapidity in the nucleon-nucleon centre-of-mass. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward asymmetry for phi-meson production is measured for $2.96&lt;|y|&lt;3.53$, showing no significant $p_{\rm T}$ dependence within the uncertainties. The $p_{\rm T}$-dependence of the phi nuclear modification factor $R_{\rm pPb}$ exhibits an enhancement up to a factor 1.6 at $p_{\rm T}$ = 3-4 GeV/$c$ in the Pb-going direction. The $p_{\rm T}$-dependence of the $\phi$-meson cross section in pp collisions at $\sqrt{s}$ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for $1 &lt; p_{\rm T} &lt; 5$ GeV/$c$ and $2.5
DOI: 10.17182/hepdata.77058.v1/t1
title: "Table 1" of "Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at sqrt(s) = 8 TeV using H to WW decays"

description: The fiducial differential cross section in each Higgs pT bin. The first uncertainty is the total (stat+syst) uncertainty. The second is the statistical uncertainty and the third and fourth are Type A and Type B systematic uncertainties, respectively. The last one is the model dependence uncertainty (Type C).
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; W + W - decay mode, followed by leptonic decays of the W bosons to an oppositely charged electron-muon pair in the final state. The measurements are performed using data collected by the CMS experiment at the LHC at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.4 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the lepton pair pT and missing pT . The differential cross section times branching fraction is measured as a function of the Higgs boson pT in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. The production cross section times branching fraction in the fiducial phase space is measured to be 39 +/- 8 (stat) +/- 9 (syst) fb. The measurements are found to agree, within experimental uncertainties, with theoretical calculations based on the standard model. 

The fiducial region is defined at particle level (using Born level leptons) as:

- emununu
- leading lepton pT &gt; 20 GeV
- subleading lepton pT &gt; 10 GeV
- psudorapidity of electrons and muons |eta| &lt; 2.5
- Invariant mass of the two charged leptons mll &gt; 12 GeV
- Charged lepton pair pT &gt; 30 GeV
- Invariant mass of the leptonic system in the transverse plane mT(emununu) &gt; 50 GeV
DOI: 10.17182/hepdata.77058.v1/t2
title: "Table 2" of "Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at sqrt(s) = 8 TeV using H to WW decays"

description: The measured total cross section in the fiducial region. The first systematic uncertainty is the statistical uncertainty and the second is the systematic.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; W + W - decay mode, followed by leptonic decays of the W bosons to an oppositely charged electron-muon pair in the final state. The measurements are performed using data collected by the CMS experiment at the LHC at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.4 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the lepton pair pT and missing pT . The differential cross section times branching fraction is measured as a function of the Higgs boson pT in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. The production cross section times branching fraction in the fiducial phase space is measured to be 39 +/- 8 (stat) +/- 9 (syst) fb. The measurements are found to agree, within experimental uncertainties, with theoretical calculations based on the standard model. 

The fiducial region is defined at particle level (using Born level leptons) as:

- emununu
- leading lepton pT &gt; 20 GeV
- subleading lepton pT &gt; 10 GeV
- psudorapidity of electrons and muons |eta| &lt; 2.5
- Invariant mass of the two charged leptons mll &gt; 12 GeV
- Charged lepton pair pT &gt; 30 GeV
- Invariant mass of the leptonic system in the transverse plane mT(emununu) &gt; 50 GeV
DOI: 10.17182/hepdata.77058.v1/t3
title: "Table 3" of "Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at sqrt(s) = 8 TeV using H to WW decays"

description: Correlation matrix among the Higgs pT bins of the differential spectrum.
description: CERN-LHC.The cross section for Higgs boson production in pp collisions is studied using the H -&gt; W + W - decay mode, followed by leptonic decays of the W bosons to an oppositely charged electron-muon pair in the final state. The measurements are performed using data collected by the CMS experiment at the LHC at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.4 fb^-1 . The Higgs boson transverse momentum (pT) is reconstructed using the lepton pair pT and missing pT . The differential cross section times branching fraction is measured as a function of the Higgs boson pT in a fiducial phase space defined to match the experimental acceptance in terms of the lepton kinematics and event topology. The production cross section times branching fraction in the fiducial phase space is measured to be 39 +/- 8 (stat) +/- 9 (syst) fb. The measurements are found to agree, within experimental uncertainties, with theoretical calculations based on the standard model. 

The fiducial region is defined at particle level (using Born level leptons) as:

- emununu
- leading lepton pT &gt; 20 GeV
- subleading lepton pT &gt; 10 GeV
- psudorapidity of electrons and muons |eta| &lt; 2.5
- Invariant mass of the two charged leptons mll &gt; 12 GeV
- Charged lepton pair pT &gt; 30 GeV
- Invariant mass of the leptonic system in the transverse plane mT(emununu) &gt; 50 GeV
DOI: 10.17182/hepdata.77059.v1/t1
title: "Table 1" of "Search for heavy Majorana neutrinos in e+/- e+/- plus jets and e+/- mu+/- plus jets events in proton-proton collisions at sqrt(s) = 8 TeV"

description: Selection requirements for the low- and high-mass signal regions.
description: Numbers taken from Tables 1-7 of arXiv:1603.02248v2.
DOI: 10.17182/hepdata.77059.v1/t2
title: "Table 2" of "Search for heavy Majorana neutrinos in e+/- e+/- plus jets and e+/- mu+/- plus jets events in proton-proton collisions at sqrt(s) = 8 TeV"

description: ee channel. Selection requirements on discriminating variables determined by the optimization for each Majorana neutrino mass point. The last column shows the overall signal acceptance. Different selection criteria are used for low- and high-mass search regions. The "-" indicates that no selection requirement is made.
description: Numbers taken from Tables 1-7 of arXiv:1603.02248v2.