cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.114866.v1/t19
title: "Background Covariance Matrix (e channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Covariance matrix for all bins used in the background-only fit of the electron channel of this analysis. There are 243 bins in total, 81 for every data-taking year. For every year, each region has nine bins and the bins are grouped by rergion in the following order: ee boosted DY CR, #mu-jet flavor CR, ee resolved DY CR, resolved flavor CR, ee boosted SR, ee resolved SR, #mu#mu boosted DY CR, e-jet flavor CR, and #mu#mu resolved DY CR.
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/t20
title: "Background Covariance Matrix (mu channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Covariance matrix for all bins used in the background-only fit of the muon channel of this analysis. There are 243 bins in total, 81 for every data-taking year. For every year, each region has nine bins and the bins are grouped by rergion in the following order: ee boosted DY CR, #mu-jet flavor CR, ee resolved DY CR, #mu#mu boosted DY CR, e-jet flavor CR, $#mu#mu$ resolved DY CR, resolved flavor CR, #mu#mu boosted SR, and the #mu#mu resolved SR.
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/t17
title: "Cross section limits vs WR and N mass ($\mu$ channel)" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 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 muon 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/t21
title: "Cut-flow table mN=0.2TeV, boosted, e channel, 2016" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predicted signal yields for the 2016 data-taking period, corresponding to $35.9\,\text{fb}^{-1}$, after the application of each search requirement for the $m_{W_{R}} = 0.3$, 0.4, and 0.5 TeV and $m_{N} = 0.2$ TeV signal hypotheses for the boosted , dielectron channel.The requirements listed are cumulative such that only the events and objects passing a given requirement are considered in subsequent requirements.
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/t22
title: "Cut-flow table (mWR,mN)=(3.0,1.4)TeV, resolved, e channel, 2016" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predicted signal yields for the 2016 data-taking period, corresponding to $35.9\,\text{fb}^{-1}$, after the application of each search requirement for the $(m_{W_{R}},m_{N}) = (3.0,1.4)$ TeV signal hypothesis for the resolved , dielectron channel.The requirements listed are cumulative such that only the events and objects passing a given requirement are considered in subsequent requirements.
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/t23
title: "Cut-flow table (mWR,mN)=(4.0,2.0)TeV, resolved, e channel, 2016" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predicted signal yields for the 2016 data-taking period, corresponding to $35.9\,\text{fb}^{-1}$, after the application of each search requirement for the $(m_{W_{R}},m_{N}) = (4.0,2.0)$ TeV signal hypothesis for the resolved , dielectron channel.The requirements listed are cumulative such that only the events and objects passing a given requirement are considered in subsequent requirements.
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/t26
title: "Cut-flow table (mWR,mN)=(3.0,1.4)TeV, resolved, mu channel, 2016" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predicted signal yields for the 2016 data-taking period, corresponding to $35.9\,\text{fb}^{-1}$, after the application of each search requirement for the $(m_{W_{R}},m_{N}) = (3.0,1.4)$ TeV signal hypothesis for the resolved , dimuon channel.The requirements listed are cumulative such that only the events and objects passing a given requirement are considered in subsequent requirements.
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: 10.25549/vercoutere-ouc110610477
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/t24
title: "Cut-flow table (mWR,mN)=(5.0,3.0)TeV, resolved, e channel, 2016" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predicted signal yields for the 2016 data-taking period, corresponding to $35.9\,\text{fb}^{-1}$, after the application of each search requirement for the $(m_{W_{R}},m_{N}) = (5.0,3.0)$ TeV signal hypothesis for the resolved , dielectron channel.The requirements listed are cumulative such that only the events and objects passing a given requirement are considered in subsequent requirements.
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/t25
title: "Cut-flow table mN=0.2TeV, boosted, mu channel, 2016" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predicted signal yields for the 2016 data-taking period, corresponding to $35.9\,\text{fb}^{-1}$, after the application of each search requirement for the $m_{W_{R}} = 0.3$, 0.4, and 0.5 TeV and $m_{N} = 0.2$ TeV signal hypotheses for the boosted , dimuon channel.The requirements listed are cumulative such that only the events and objects passing a given requirement are considered in subsequent requirements.
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/t28
title: "Cut-flow table (mWR,mN)=(5.0,3.0)TeV, resolved, mu channel, 2016" of "Search for a right-handed W boson and a heavy neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Predicted signal yields for the 2016 data-taking period, corresponding to $35.9\,\text{fb}^{-1}$, after the application of each search requirement for the $(m_{W_{R}},m_{N}) = (5.0,3.0)$ TeV signal hypothesis for the resolved , dimuon channel.The requirements listed are cumulative such that only the events and objects passing a given requirement are considered in subsequent requirements.
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.