cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.130266.v1/t46
title: "Aux Figure 24f (Observed)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Observed negative log-likelihood scans as a function of $\kappa_{\mu}$.
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc110611297
title: 2 nude women plus woman in a black skirt

description: Back view of one creamish orange nude female outlined in brown and depicted from shoulders to ankles; she is standing in front of a nude blue female (?) who is facing her and is depicted from shoulders to ankles. Behind the blue female stands a female in a short black skirt with brown legs and black shoes depicted from the back from the waist to feet. The multi-colored background includes vertical, square, and diagonal designs. The letters AD are on an orange patch. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130266.v1/t47
title: "Aux Figure 24g (Expected)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Expected negative log-likelihood scans as a function of $\kappa_{g}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t48
title: "Aux Figure 24g (Observed)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Observed negative log-likelihood scans as a function of $\kappa_{g}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t49
title: "Aux Figure 24h (Expected)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Expected negative log-likelihood scans as a function of $\kappa_{\gamma}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t50
title: "Aux Figure 24h (Observed)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Observed negative log-likelihood scans as a function of $\kappa_{\gamma}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t51
title: "Aux Figure 24i (Expected)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Expected negative log-likelihood scans as a function of $\kappa_{Z\gamma}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t52
title: "Aux Figure 24i (Observed)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Observed negative log-likelihood scans as a function of $\kappa_{Z\gamma}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t53
title: "Aux Figure 24j (Expected)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Expected negative log-likelihood scans as a function of $B_{inv.}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t54
title: "Aux Figure 24j (Observed)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Observed negative log-likelihood scans as a function of $B_{inv.}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t55
title: "Aux Figure 24k (Expected)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Expected negative log-likelihood scans as a function of $B_{u.}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t56
title: "Aux Figure 24k (Observed)" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: Observed negative log-likelihood scans as a function of $B_{u.}$.
description: No data abstract available.
DOI: 10.17182/hepdata.130266.v1/t57
title: "STXS acceptances" of "A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery"

description: The acceptances of STXS stage 1.2 kinematic regions in the Higgs boson production processes.
description: No data abstract available.
DOI: 10.17182/hepdata.130268.v1/t1
title: "Table 1" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential production cross section in $\eta &gt; 10.75$
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130268.v1/t2
title: "Table 2" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential production cross section in $10.06 &lt; \eta &lt; 10.75$
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130268.v1/t3
title: "Table 3" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential production cross section in $9.65 &lt; \eta &lt; 10.06$
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130268.v1/t4
title: "Table 4" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential production cross section in $8.99 &lt; \eta &lt; 9.21$
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130268.v1/t5
title: "Table 5" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential production cross section in $8.80 &lt; \eta &lt; 8.99$
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130268.v1/t6
title: "Table 6" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential production cross section in $8.65 &lt; \eta &lt; 8.80$
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.25549/vercoutere-ouc110611313
title: Green staircase

description: Street scene with two yellowish green buildings outlined in gree with a street and sidewalk between the buildings. One building has a green staircase coming down from inside the building. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130268.v1/t7
title: "Table 7" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential energy flow vs pseudorapidity
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130268.v1/t8
title: "Table 8" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive differential production cross section vs pseudorapidity
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130268.v1/t9
title: "Table 9" of "Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\mathrm{\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector"

description: Neutron (and antineutron) inclusive production cross section vs elasticity
description: Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\mathrm{\sqrt{s} = 13\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\eta &gt; 10.75$, $10.06 &lt; \eta &lt; 10.75$, $9.65 &lt; \eta &lt; 10.06$, $8.99 &lt; \eta &lt; 9.21$, $8.80 &lt; \eta &lt; 8.99$ and $8.65 &lt; \eta &lt; 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\mathrm{c \tau&lt;1\,cm}$).
DOI: 10.17182/hepdata.130491.v1/t1
title: "Upper limits on the charged Higgs boson mass" of "Search for a charged Higgs boson decaying into a heavy neutral Higgs boson and a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits at 95% CL on the product of cross section and branching fraction as a function of mH+ and assuming mH = 200 GeV for the combination of all final states considered.
description: CERN-LHC. Search for charged Higgs bosons H+ decaying into a heavy neutral Higgs boson H and a W boson. The analysis targets the H decay into a pair of tau leptons with at least one of them decaying hadronically and with an additional electron or muon present in the event. The search is based on proton-proton collision data recorded by the CMS experiment during 2016-2018 at a center-of-mass energy of 13 TeV (138 fb^-1, 2016--2018) with the CMS experiment. The data are consistent with standard model background expectations. Upper limits at 95% confidence level are set on the product of the cross section and branching fraction for an H+ (or H-) in the mass range of 300-700 GeV, assuming an H with a mass of 200 GeV. The observed limits range from 0.085 pb for an H+ mass of 300 GeV to 0.019 pb for a mass of 700 GeV. These are the first limits on H+ production in the H+ to HW+ decay channel at the LHC.
DOI: 10.17182/hepdata.130562.v1/t1
title: "Table1" of "Observation of same-sign WW production from double parton scattering in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured values of inclusive and fiducial cross section for same-sign WW bosons via DPS
description: The first observation of the production of WpmWpm bosons from double parton scattering processes using same-sign electron-muon and dimuon events in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 138 invfb recorded at a center-of-mass energy of 13 TeV using the CMS detector at the CERN LHC. Multivariate discriminants are used to distinguish the signal process from the main backgrounds. A binned maximum likelihood fit is performed to extract the signal cross section. The measured cross section for production of same-sign W bosons decaying leptonically is 80.7 +/- 11.2 (stat) {+9.5}{-8.6} (syst) +/- 12.1 (model) fb, whereas the measured fiducial cross section is 6.28 +/- 0.81 (stat) +/- 0.69 (syst) +/- 0.37 (model) fb. The observed significance of the signal is 6.2 standard deviations above the background-only hypothesis.
DOI: 10.17182/hepdata.130562.v1/t2
title: "Table2" of "Observation of same-sign WW production from double parton scattering in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Effective DPS cross section paramater
description: The first observation of the production of WpmWpm bosons from double parton scattering processes using same-sign electron-muon and dimuon events in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 138 invfb recorded at a center-of-mass energy of 13 TeV using the CMS detector at the CERN LHC. Multivariate discriminants are used to distinguish the signal process from the main backgrounds. A binned maximum likelihood fit is performed to extract the signal cross section. The measured cross section for production of same-sign W bosons decaying leptonically is 80.7 +/- 11.2 (stat) {+9.5}{-8.6} (syst) +/- 12.1 (model) fb, whereas the measured fiducial cross section is 6.28 +/- 0.81 (stat) +/- 0.69 (syst) +/- 0.37 (model) fb. The observed significance of the signal is 6.2 standard deviations above the background-only hypothesis.
DOI: 10.17182/hepdata.130708.v1/t1
title: "Born cross-section" of "Precision measurements of the timelike electromagnetic form factors of pion, kaon, and proton."

description: Born cross section of $e^+e^-\rightarrow h^+h^-$
description: A precise measurement of the cross section of the process $e^+e^- \to \pi^+\pi^-(\gamma)$ from threshold to an energy of $3$ GeV is obtained with the initial-state radiation (ISR) method using $232$ fb$^{-1}$ of data collected with the BaBar detector at $e^+e^-$ center-of-mass energies near $10.6$ GeV. The ISR luminosity is determined from a study of the leptonic process $e^+e^-\to\mu^+\mu^-(\gamma)\gamma_{\rm ISR}$, which is found to agree with the next-to-leading-order QED prediction to within 1.1\%. The cross section for the process $e^+e^-\to\pi^+\pi^-(\gamma)$ is obtained with a systematic uncertainty of 0.5\% in the dominant $\rho$ resonance region. The leading-order hadronic contribution to the muon magnetic anomaly calculated using the measured $\pi\pi$ cross section from threshold to $1.8$ GeV is $(514.1 \pm 2.2({\rm stat}) \pm 3.1({\rm syst}))\times 10^{-10}$.
DOI: 10.17182/hepdata.130708.v1/t2
title: "Timelike form factor" of "Precision measurements of the timelike electromagnetic form factors of pion, kaon, and proton."

description: Timelike form factor
description: A precise measurement of the cross section of the process $e^+e^- \to \pi^+\pi^-(\gamma)$ from threshold to an energy of $3$ GeV is obtained with the initial-state radiation (ISR) method using $232$ fb$^{-1}$ of data collected with the BaBar detector at $e^+e^-$ center-of-mass energies near $10.6$ GeV. The ISR luminosity is determined from a study of the leptonic process $e^+e^-\to\mu^+\mu^-(\gamma)\gamma_{\rm ISR}$, which is found to agree with the next-to-leading-order QED prediction to within 1.1\%. The cross section for the process $e^+e^-\to\pi^+\pi^-(\gamma)$ is obtained with a systematic uncertainty of 0.5\% in the dominant $\rho$ resonance region. The leading-order hadronic contribution to the muon magnetic anomaly calculated using the measured $\pi\pi$ cross section from threshold to $1.8$ GeV is $(514.1 \pm 2.2({\rm stat}) \pm 3.1({\rm syst}))\times 10^{-10}$.
DOI: 10.25549/vercoutere-ouc110611319
title: Nude women standing beside a white star and black ball

description: One yellow female outlined in red with orange hair standing outside in front of an orange building with gray multi-paned windows; a white star and a black ball float to the right of the female; background is green floor and blue street. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130712.v1/t1
title: "xsec_diff_mjet" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The particle-level $\mathrm{t}\overline{\mathrm{t}}$ differential cross section in the fiducial region as a function of the XCone-jet mass.
description: A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton+jets channel of top quark pair production ($\mathrm{t}\overline{\mathrm{t}}$) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than $400\,\mathrm{GeV}$. The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of $138\,\mathrm{fb}^{-1}$. The differential $\mathrm{t}\overline{\mathrm{t}}$ production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.17182/hepdata.130712.v1/t2
title: "correlations_xsec_diff_mjet" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlations between bins in the particle-level $\mathrm{t}\overline{\mathrm{t}}$ differential cross section as a function of the XCone-jet mass.
description: A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton+jets channel of top quark pair production ($\mathrm{t}\overline{\mathrm{t}}$) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than $400\,\mathrm{GeV}$. The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of $138\,\mathrm{fb}^{-1}$. The differential $\mathrm{t}\overline{\mathrm{t}}$ production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of $173.06 \pm 0.84\,\mathrm{GeV}$.