cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93063.v1/t3
title: "Table 3" of "Measurement of differential cross sections for single diffractive dissociation in $\sqrt{s} = 8$ TeV $pp$ collisions using the ATLAS ALFA spectrometer"

description: Hadron-level differential SD cross section as a function of log_10 xi.
description: A dedicated sample of Large Hadron Collider proton-proton collision data at centre-of-mass energy s√=8 TeV is used to study inclusive single diffractive dissociation, pp→Xp. The intact final-state proton is reconstructed in the ATLAS ALFA forward spectrometer, while charged particles from the dissociated system X are measured in the central detector components. Cross sections are measured differentially as functions of the proton fractional energy loss ξ, the squared four-momentum transfer t, and Δη, a variable that characterises the rapidity gap separating the proton and the system X. The data are consistent with an exponential t dependence, dσ/dt∝eBt with slope parameter B=7.65±0.34 GeV−2. Interpreted in the framework of Regge phenomenology, the ξ dependence leads to a pomeron intercept of α(0)=1.07±0.09.
DOI: 10.17182/hepdata.93064.v1/t1
title: "Table 1: Mass measurements" of "Study of excited $\Lambda_\mathrm{b}^0$ states decaying to $\Lambda_\mathrm{b}^0\pi^+\pi^-$ in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Measured masses
description: CERN-LHC-CMS. Studies of excited Lambda-b states in their decays into Lambda-b pi+ pi- in pp collisions at sqrt(s)=13 TeV.
DOI: 10.17182/hepdata.93064.v1/t2
title: "Table 2: Mass difference measurements" of "Study of excited $\Lambda_\mathrm{b}^0$ states decaying to $\Lambda_\mathrm{b}^0\pi^+\pi^-$ in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Measured mass differences
description: CERN-LHC-CMS. Studies of excited Lambda-b states in their decays into Lambda-b pi+ pi- in pp collisions at sqrt(s)=13 TeV.
DOI: 10.17182/hepdata.93065.v1/t1
title: "Table 1: Results for the braching fraction ratio" of "Observation of the $\Lambda_\mathrm{b}^0 \to$ J/$\psi \Lambda \phi$ decay in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: The measured ratio of branching fractions
description: CERN-LHC-CMS. Observation of the Lambda-b to J/psi Lambda phi decay in proton-proton collisions at sqrt(s)= 13 TeV.
DOI: 10.17182/hepdata.93067.v1/t1
title: "Figure 1" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Reconstructed distribution of $m_\mathrm{jet}$ after the full event selection in the lepton+jets channel.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t2
title: "Figure 2 a" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp 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 is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t3
title: "Figure 2 b" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The normalized 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 is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t4
title: "Figure 2a Stat Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the statistical uncertainties of Figure 2a is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t5
title: "Figure 2a Experimental Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the experimental uncertainties of Figure 2a is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t6
title: "Figure 2a Model Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the model uncertainties of Figure 2a is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t7
title: "Figure 2b Stat Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the statistical uncertainties of Figure 2b is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t8
title: "Figure 2b Experimental Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the experimental uncertainties of Figure 2b is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v1/t9
title: "Figure 2b Model Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the model uncertainties of Figure 2b is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v2/t1
title: "Figure 2 a" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp 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 is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93013.v1/t13
title: "RpPb D*, Figure 8 " of "Measurement of prompt D$^0$, D$^+$, D$^{*+}$, and D$^+_s$ production in p$-$Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$"

description: $R_{\rm{pPb}}$ of prompt D* mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.93013.v1/t14
title: "RpPb D+, Figure 8" of "Measurement of prompt D$^0$, D$^+$, D$^{*+}$, and D$^+_s$ production in p$-$Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$"

description: $R_{\rm{pPb}}$ of prompt D+ mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.93067.v2/t2
title: "Figure 2 b" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The normalized 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 is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v2/t3
title: "Figure 2a Stat Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the statistical uncertainties of Figure 2a is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v2/t4
title: "Figure 2a Experimental Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the experimental uncertainties of Figure 2a is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.
DOI: 10.17182/hepdata.93067.v2/t5
title: "Figure 2a Model Covariances" of "Measurement of the jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at $\sqrt{s} =$ 13 TeV"

description: The covariance matrix containing the model uncertainties of Figure 2a is shown.
description: A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in \pp collisions at $\sqrt{s}=13\,\mathrm{TeV}$. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of $35.9\,\mathrm{fb}^{-1}$. The measurement is performed in the lepton+jets channel of $\mathrm{t}\overline{\mathrm{t}}$ events, where the lepton is an electron or muon. The products of the hadronic top quark decay $\mathrm{t} \rightarrow \mathrm{b}\mathrm{W} \rightarrow \mathrm{b}\mathrm{q}\mathrm{q}'$ are reconstructed as a single jet with transverse momentum larger than $400\,\mathrm{GeV}$. The $\mathrm{t}\overline{\mathrm{t}}$ cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of $172.6 \pm 2.5\,\mathrm{GeV}$. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of three relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements.