cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.130712.v1/t3
title: "covariance_stat_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 covariance matrix containing the statistical uncertainties of 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 $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.17182/hepdata.130712.v1/t4
title: "covariance_exp_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 covariance matrix containing the experimental uncertainties of 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 $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.17182/hepdata.130712.v1/t5
title: "covariance_model_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 covariance matrix containing the model uncertainties of 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 $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.17182/hepdata.130712.v1/t6
title: "xsec_diff_norm_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 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 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/t10
title: "covariance_model_xsec_diff_norm_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 covariance matrix containing the model uncertainties of the normalized 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 $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.17182/hepdata.130712.v1/t7
title: "correlations_xsec_diff_norm_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 normalized 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 $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.17182/hepdata.130712.v1/t8
title: "covariance_stat_xsec_diff_norm_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 covariance matrix containing the statistical uncertainties of the normalized 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 $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.17182/hepdata.130712.v1/t9
title: "covariance_exp_xsec_diff_norm_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 covariance matrix containing the experimental uncertainties of the normalized 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 $173.06 \pm 0.84\,\mathrm{GeV}$.
DOI: 10.25549/vercoutere-ouc110611336
title: 2 nude women and three numerals

description: One white nude female outlined in yellow is reclining beneath a "flesh" colored nude female who is standing and walking towards the right of the painting. One side of the painting is green; the remainder of the background is blank with three numerals (7, 16, and, 45) and other symbols in black. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130712.v1/t11
title: "uncertainties_exp" 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: Relative experimental uncertainties of 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/t12
title: "uncertainties_model" 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: Relative model uncertainties of 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/t13
title: "uncertainties_norm_exp" 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: Relative experimental uncertainties of 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 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/t14
title: "uncertainties_norm_model" 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: Relative model uncertainties of 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 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.130726.v1/t1
title: "Table 1" of "Search for Higgs boson decays into Z and J/$\psi$ and for Higgs and Z boson decays into J/$\psi$ or $\Upsilon$ pairs in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Exclusion limits at 95% CL on the branching fractions ($\mathcal{B}$s) of the $H$ and $Z$ boson decays. The second column lists the observed limits for the case that both intermediate particles are longitudinally polarized. The third column shows the median expected limits with the upper and lower bounds in the expected 68% CL intervals. The last two columns list observed upper limits for unpolarized and transversely polarized intermediate particles.
description: Decays of the Higgs boson into a $Z$ boson and a $J/\psi$ or $\psi(2S)$ meson are searched for in four-lepton final states with the CMS detector at the LHC. A data set of proton-proton collisions corresponding to an integrated luminosity of 138 $fb^{-1}$ is used. Using the same data set, decays of the Higgs and $Z$ boson into quarkonium pairs are also searched for. An observation of such decays with this sample would indicate the presence of physics beyond the standard model. No evidence for these decays has been observed and upper limits at the 95\% confidence level are placed on the corresponding branching fractions ($\mathcal{B}$). Assuming longitudinal polarization of the Higgs boson decay products, 95\% confidence level observed upper limits for $\mathcal{B}(H \to Z J/\psi)$ and $\mathcal{B}(H\to Z \psi(2S))$ are $1.9\times 10^{-3}$ and $6.6\times 10^{-3}$, respectively.
DOI: 10.25549/vercoutere-ouc110611346
title: Green nude woman reclining diagonally

description: One nude green and yellow female outlined in brown with brown nipples and pubic area is depicted from head to calves. She is leaning on a brown hollow cynlinder The background has brown netting and a turquoise, blue, white. and red floor. See description of 001 for OT notes.
DOI: 10.25549/vercoutere-ouc110611367
title: 3 nude women in green, white, and dark gray

description: Three nude females: one in green outlined in black with a black belly button and pubic region and white shading on legs depicted from chest to knees is standing; one in dark gray with white breasts, arms, and pubic area depicted from breasts to calves is standing, and one in white and black is lying on her back with one leg bent up between the other two. See description of 001 for OT notes.
DOI: 10.25549/vercoutere-ouc110611362
title: Dressed woman with 4 nude women in pink, purple, blue, and yellow

description: One female dressed in a long-sleeved black and white striped blouse and black skirt depicted from head to hips is standing in front of four seated nude females depicted from neck to knees: one is pink outlined in red, one is dark purple depicted from neck to waist, one is blue with black nipples, and one is yellow with black nipples and pubic region. Background is dark brown, black, red, with a white and black grid cloth between the blue and yellow figures. See description of 001 for OT notes.
DOI: 10.25549/vercoutere-ouc110611379
title: Nude green and orange woman crouching

description: One green and orange female with black nipples depicted from head to toes is crouching in an outdoors scene with a green tree; gray mountain in the distance; orange, blue, and green ground. Two large maroon bowls are beside the figure. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130771.v1/t1
title: "Born cross-section" of "High Precision Measurements of the Form Factors of Pion, Kaon, and Proton at Large Timelike Momentum Transfers"

description: Born cross section of $e^+e^-\rightarrow h^+h^-$
description: The electromagnetic structure of the lightest hadrons, proton, pion, and kaon is studied by high-precision measurements of their form factors for the highest timelike momentum transfers of $|Q^2|=s=14.2$ and 17.4 GeV$^2$. Data taken with the CLEO-c detector at $\sqrt{s}=3.772$ and 4.170 GeV, with integrated luminosities of 805 and 586 pb$^{-1}$, respectively, have been used to study $e^+e^-$ annihilations into $\pi^+\pi^-$, $K^+K^-$, $p\bar{p}$. The dimensional counting rule prediction that at large $Q^2$ the quantity $Q^2F(Q^2)$ for pseudoscalar mesons is nearly constant, and should vary only weakly as the strong coupling constant $\alpha_S(Q^2)$ is confirmed for both pions and kaons. However, the measurements are in strong quantitative disagreement with the predictions of the existing quantum chromodynamics-based models. For protons, it is found that the timelike form factors continue to remain nearly twice as large as the corresponding spacelike form factors measured in electron elastic scattering, in significant violation of the expectation of their equality at large $Q^2$. Further, in contrast to pions and kaons, a significant difference is observed between the values of the corresponding quantity $|Q^4|G_M(|Q^2|)/\mu_p$ for protons at $|Q^2|=14.2$ and 17.4 GeV$^2$. The results suggest the constancy of $|Q^2|G_M(|Q^2|)/\mu_p$, instead, at these large $|Q^2|$.