cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.25549/vercoutere-ouc110610472
title: 2 women lying down with arms stretched out to each other plus word salad

description: One orange nude female with blond hair lying on her stomach with one leg bent and one leg stretched out, her head is towards the bottom of the page, and her arms are raised above her head; one pink, orange, and yellow nude female with orange face and orange hair lying on her stomach with one leg bent at the knee and the other stretched out, one arm stretched out toward the other woman, her head is at the top of the page; the area between the legs is turquoise or green; area around head and feet is pink; the remainder of the page is a word salad printed in red around the figures, including some words on the left side that are perpendicular to the other words on an unpainted background. See description of 347 for OT notes.
DOI: 10.17182/hepdata.114866.v1/t10
title: "Invariant mass distribution in the boosted SR electron channel" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $m_{lJ}$ distribution in the boosted signal region, electron channel.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t12
title: "Cross section limits vs WR mass ($m_{N}=0.5m_{WR}$,e channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The expected and observed $95\%$ CL upper limits on the production cross section times the branching fraction $\sigma (\mathrm{p}\mathrm{p} \rightarrow W_{R}) \mathcal{B}(W_{R} \rightarrow \mathrm{e}\mathrm{e}\mathrm{q}\overline{\mathrm{q}'})$ for $m_{N} = m_{W_{R}}/2$ GeV in the electron channel. The red solid lines represent the values expected from the theory.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t13
title: "Cross section limits vs WR mass($m_{N}=0.5m_{WR}$,$\mu$ channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The expected and observed $95\%$ CL upper limits on the production cross section times the branching fraction $\sigma (\mathrm{p}\mathrm{p} \rightarrow W_{R}) \mathcal{B}(W_{R} \rightarrow \mathrm{e}\mathrm{e}\mathrm{q}\overline{\mathrm{q}'})$ for $m_{N} = m_{W_{R}}/2$ GeV in the muon channel. The red solid lines represent the values expected from the theory.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t14
title: "Cross section limits vs WR mass ($m_{N}=200$ GeV, e channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The expected and observed $95\%$ CL upper limits on the production cross section times the branching fraction $\sigma (\mathrm{p}\mathrm{p} \rightarrow W_{R}) \mathcal{B}(W_{R} \rightarrow \mathrm{e}\mathrm{e}\mathrm{q}\overline{\mathrm{q}'})$ for $m_{N} = 200$ GeV in the electron channel. The red solid lines represent the values expected from the theory.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t7
title: "Invariant mass distribution in the boosted flavor CR muon jet" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $m_{lJ}$ distribution in the boosted flavor control region, with muon jet
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t8
title: "Invariant mass distribution in the resolved SR electron channel" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $m_{lljj}$ distribution in the resolved signal region, electron channel.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t9
title: "Invariant mass distribution in the resolved SR muon channel" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $m_{lljj}$ distribution in the resolved signal region, muon channel.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t11
title: "Invariant mass distribution in the boosted SR muon channel" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $m_{lJ}$ distribution in the boosted signal region, muon channel.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t15
title: "Cross section limits vs WR mass ($m_{N}=200$ GeV, $\mu$ channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The expected and observed $95\%$ CL upper limits on the production cross section times the branching fraction $\sigma (\mathrm{p}\mathrm{p} \rightarrow W_{R}) \mathcal{B}(W_{R} \rightarrow \mathrm{e}\mathrm{e}\mathrm{q}\overline{\mathrm{q}'})$ for $m_{N} = 200$ GeV in the muon channel. The red solid lines represent the values expected from the theory.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t16
title: "Cross section limits vs WR and N mass (e channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The observed $95\%$ CL upper limits on the production cross section times the branching fraction $\sigma (\mathrm{p}\mathrm{p} \rightarrow W_{R}) \mathcal{B}(W_{R} \rightarrow \mathrm{e}\mathrm{e}\mathrm{q}\overline{\mathrm{q}'})$ divided by the theory cross sections in the electron channel. The observed exclusions are shown for the resolved (solid green), boosted (solid blue), and combined (solid black) channels, along with the expected exclusion for the combined result (dotted black). The dash-dotted lines represent the one standard deviation of the expected exclusion. The observed exclusions from the previous search performed by the CMS Collaboration (arXiv:1803.11116) is also shown in magenta.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.
DOI: 10.17182/hepdata.114866.v1/t18
title: "Relative unertainties on total yields" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Relative uncertainties in the total yields of the signal and background predictions.
description: A search for a right-handed $\mathrm{W}$ boson ($\mathrm{W_R}$) and a heavy neutrino ($\mathrm{N}$), in a final state consisting of two same--flavor leptons ($\mathrm{e}\mathrm{e}$ or $\mu\mu$) and two quarks, is presented. The search is performed with the CMS experiment at the CERN LHC using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 137 $\mathrm{fb}^{-1}$. The search covers both regions of phase space where the decay products of the heavy neutrino are merged into a single large-area jet and where the decay products are well separated. The expected signal is characterized by an excess in the invariant mass distribution of the final-state objects and no significant excess over the standard model background expectations is observed. The observations are interpreted as upper limits on the product of $\mathrm{W_R}$ production cross sections and branching fractions assuming that couplings are identical to those of the standard model $\mathrm{W}$ boson. For $m_{\mathrm{N}}=1/2~m_{\mathrm{W_R}}$ ($m_{\mathrm{N}}=200$ GeV), the mass of the $\mathrm{W_R}$ is excluded at 95\% confidence level up to 4.7 (4.8) and 5.0 (5.4) TeV for the electron and muon channels, respectively. The maximum observed global significance is in the electron channel and correpsonds to 2.78 standard deviations for a signal with $(m_{\mathrm{W_R}}, m_{\mathrm{N}}) = (6.0, 0.8)$ TeV. This analysis provides the most stringent limits on the $\mathrm{W_R}$ mass to date.