cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141455.v1/t66
title: "Figure 8" of "Search for a high-mass dimuon resonance produced in association with b quark jets at $\sqrt{s}$=13 TeV"

description: Exclusion limits at $95\%$ CL in the $|g_{\mathrm{Z'}}|$--$m_{\mathrm{Z'}}$ plane for the $B_{3}\!-\!L_{2}$ model from JHEP 04 (2023) 033, for a fixed value of $\theta_{23}=0$. The solid black (dashed red) curve represents the observed (median expected) exclusion. The dotted curve denotes the coupling values at which the $\mathrm{Z'}$ width equals one half of the $\mu\mu$ invariant mass resolution. For larger values of the couplings, the narrow width approximation intrinsic to the search strategy is not considered valid. The region enclosed between the solid black (dashed red) and the dotted curves is (expected to be) excluded. The shaded blue area represents the $|g_{\mathrm{Z'}}|$ range preferred from a global fit in JHEP 04 (2023) 033 at $95\%$ CL.
description: A search for high-mass dimuon resonance production in association with one or more $\mathrm{b}$ quark jets is presented. The study uses proton-proton collision data collected with the CMS detector at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a center-of-mass energy of $13~\mathrm{TeV}$. Model-independent limits are derived on the number of signal events with exactly one or more than one $\mathrm{b}$ quark jet. Results are also interpreted in a lepton-flavor-universal model with $\mathrm{Z'}$ boson couplings to a $\mathrm{bb}$ quark pair ($g_{\mathrm{b}}$), an $\mathrm{sb}$ quark pair ($g_{\mathrm{b}}\delta_{\mathrm{bs}}$), and any same-flavor charged lepton ($g_{\ell}$) or neutrino pair ($g_{\nu}$), with $|g_{\nu}|=|g_{\ell}|$. For a $\mathrm{Z'}$ boson with a mass $m_{\mathrm{Z'}}=350~\mathrm{GeV}$ ($2~\mathrm{TeV}$) and $|\delta_{\mathrm{bs}}| &lt; 0.25$, the majority of the parameter space with $0.0057 &lt; |g_{\ell}| &lt; 0.35$ ($0.25 &lt; |g_{\ell}| &lt; 0.43$) and $0.0079 &lt; |g_{\mathrm{b}}| &lt; 0.46$ ($0.34 &lt; |g_{\mathrm{b}}| &lt; 0.57$) is excluded at $95\%$ confidence level. Finally, constraints are set on a $\mathrm{Z'}$ model with parameters consistent with low-energy $\mathrm{b} \to \mathrm{s}\ell\ell$ measurements. In this scenario, most of the allowed parameter space is excluded for a $\mathrm{Z'}$ boson with $350
DOI: 10.17182/hepdata.141455.v1/t67
title: "Figure 8, observed exclusion" of "Search for a high-mass dimuon resonance produced in association with b quark jets at $\sqrt{s}$=13 TeV"

description: Observed exclusion limits at $95\%$ CL in the $|g_{\mathrm{Z'}}|$--$m_{\mathrm{Z'}}$ plane for the $B_{3}\!-\!L_{2}$ model from JHEP 04 (2023) 033, for a fixed value of $\theta_{23}=0$.
description: A search for high-mass dimuon resonance production in association with one or more $\mathrm{b}$ quark jets is presented. The study uses proton-proton collision data collected with the CMS detector at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a center-of-mass energy of $13~\mathrm{TeV}$. Model-independent limits are derived on the number of signal events with exactly one or more than one $\mathrm{b}$ quark jet. Results are also interpreted in a lepton-flavor-universal model with $\mathrm{Z'}$ boson couplings to a $\mathrm{bb}$ quark pair ($g_{\mathrm{b}}$), an $\mathrm{sb}$ quark pair ($g_{\mathrm{b}}\delta_{\mathrm{bs}}$), and any same-flavor charged lepton ($g_{\ell}$) or neutrino pair ($g_{\nu}$), with $|g_{\nu}|=|g_{\ell}|$. For a $\mathrm{Z'}$ boson with a mass $m_{\mathrm{Z'}}=350~\mathrm{GeV}$ ($2~\mathrm{TeV}$) and $|\delta_{\mathrm{bs}}| &lt; 0.25$, the majority of the parameter space with $0.0057 &lt; |g_{\ell}| &lt; 0.35$ ($0.25 &lt; |g_{\ell}| &lt; 0.43$) and $0.0079 &lt; |g_{\mathrm{b}}| &lt; 0.46$ ($0.34 &lt; |g_{\mathrm{b}}| &lt; 0.57$) is excluded at $95\%$ confidence level. Finally, constraints are set on a $\mathrm{Z'}$ model with parameters consistent with low-energy $\mathrm{b} \to \mathrm{s}\ell\ell$ measurements. In this scenario, most of the allowed parameter space is excluded for a $\mathrm{Z'}$ boson with $350
DOI: 10.17182/hepdata.141455.v1/t68
title: "Figure 8, expected exclusion" of "Search for a high-mass dimuon resonance produced in association with b quark jets at $\sqrt{s}$=13 TeV"

description: Expected exclusion limits at $95\%$ CL in the $|g_{\mathrm{Z'}}|$--$m_{\mathrm{Z'}}$ plane for the $B_{3}\!-\!L_{2}$ model from JHEP 04 (2023) 033, for a fixed value of $\theta_{23}=0$.
description: A search for high-mass dimuon resonance production in association with one or more $\mathrm{b}$ quark jets is presented. The study uses proton-proton collision data collected with the CMS detector at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a center-of-mass energy of $13~\mathrm{TeV}$. Model-independent limits are derived on the number of signal events with exactly one or more than one $\mathrm{b}$ quark jet. Results are also interpreted in a lepton-flavor-universal model with $\mathrm{Z'}$ boson couplings to a $\mathrm{bb}$ quark pair ($g_{\mathrm{b}}$), an $\mathrm{sb}$ quark pair ($g_{\mathrm{b}}\delta_{\mathrm{bs}}$), and any same-flavor charged lepton ($g_{\ell}$) or neutrino pair ($g_{\nu}$), with $|g_{\nu}|=|g_{\ell}|$. For a $\mathrm{Z'}$ boson with a mass $m_{\mathrm{Z'}}=350~\mathrm{GeV}$ ($2~\mathrm{TeV}$) and $|\delta_{\mathrm{bs}}| &lt; 0.25$, the majority of the parameter space with $0.0057 &lt; |g_{\ell}| &lt; 0.35$ ($0.25 &lt; |g_{\ell}| &lt; 0.43$) and $0.0079 &lt; |g_{\mathrm{b}}| &lt; 0.46$ ($0.34 &lt; |g_{\mathrm{b}}| &lt; 0.57$) is excluded at $95\%$ confidence level. Finally, constraints are set on a $\mathrm{Z'}$ model with parameters consistent with low-energy $\mathrm{b} \to \mathrm{s}\ell\ell$ measurements. In this scenario, most of the allowed parameter space is excluded for a $\mathrm{Z'}$ boson with $350
DOI: 10.17182/hepdata.141455.v1/t69
title: "Figure 8, $\Gamma=0.5\sigma$" of "Search for a high-mass dimuon resonance produced in association with b quark jets at $\sqrt{s}$=13 TeV"

description: Exclusion limits at $95\%$ CL in the $|g_{\mathrm{Z'}}|$--$m_{\mathrm{Z'}}$ plane for the $B_{3}\!-\!L_{2}$ model from JHEP 04 (2023) 033, for a fixed value of $\theta_{23}=0$. The coupling values are shown at which the $\mathrm{Z'}$ width equals one half of the $\mu\mu$ invariant mass resolution. For larger values of the couplings, the narrow width approximation intrinsic to the search strategy is not considered valid.
description: A search for high-mass dimuon resonance production in association with one or more $\mathrm{b}$ quark jets is presented. The study uses proton-proton collision data collected with the CMS detector at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a center-of-mass energy of $13~\mathrm{TeV}$. Model-independent limits are derived on the number of signal events with exactly one or more than one $\mathrm{b}$ quark jet. Results are also interpreted in a lepton-flavor-universal model with $\mathrm{Z'}$ boson couplings to a $\mathrm{bb}$ quark pair ($g_{\mathrm{b}}$), an $\mathrm{sb}$ quark pair ($g_{\mathrm{b}}\delta_{\mathrm{bs}}$), and any same-flavor charged lepton ($g_{\ell}$) or neutrino pair ($g_{\nu}$), with $|g_{\nu}|=|g_{\ell}|$. For a $\mathrm{Z'}$ boson with a mass $m_{\mathrm{Z'}}=350~\mathrm{GeV}$ ($2~\mathrm{TeV}$) and $|\delta_{\mathrm{bs}}| &lt; 0.25$, the majority of the parameter space with $0.0057 &lt; |g_{\ell}| &lt; 0.35$ ($0.25 &lt; |g_{\ell}| &lt; 0.43$) and $0.0079 &lt; |g_{\mathrm{b}}| &lt; 0.46$ ($0.34 &lt; |g_{\mathrm{b}}| &lt; 0.57$) is excluded at $95\%$ confidence level. Finally, constraints are set on a $\mathrm{Z'}$ model with parameters consistent with low-energy $\mathrm{b} \to \mathrm{s}\ell\ell$ measurements. In this scenario, most of the allowed parameter space is excluded for a $\mathrm{Z'}$ boson with $350
DOI: 10.17182/hepdata.141494.v1/t1
title: "Limits on Majorana HNL with muon coupling" of "Search for Majorana neutrinos in same-sign $WW$ scattering events from $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Observed and expected 95% CL upper limits on the heavy Majorana neutrino mixing element $\vert V_{\mu N} \vert^{2}$ as a function of $m_N$ in the Phenomenological Type-I Seesaw model.
description: A search for Majorana neutrinos in same-sign $W^{\pm}W^{\pm}$ scattering events is presented. The analysis uses the proton-proton collision data recorded by the ATLAS detector at $\sqrt{s}= 13$ TeV at the Large Hadron Collider during the years 2015-2018, corresponding to an integrated luminosity of 140 fb$^{-1}$. The analysis targets final states including exactly two same-sign muons and at least two hadronic jets well separated in rapidity. The modelling of the main backgrounds from Standard Model, same-sign $W^{\pm}W^{\pm}$ scattering and $WZ$ production, are constrained with data in dedicated signal-depleted control regions and the transverse momenta of the sub-leading muon is used to search for signals originating from a heavy Majorana neutrino with masses of 50 GeV to 20 TeV. The presence of a signal is examined in a signal-enriched region and is interpreted in a benchmark scenario of the Phenomenological Type I Seesaw model. In addition, the sensitivity to the Weinberg operator is investigated. No significant excess is observed over the background expectation. Upper limits at the 95% confidence level are provided on the squared muon heavy neutrino mixing element $\vert V_{\mu N} \vert^{2}$ as a function of the heavy Majorana neutrino mass $m_N$, and on the effective $\mu\mu$ Majorana neutrino mass $|m_{\mu\mu}|$.
DOI: 10.17182/hepdata.141494.v1/t2
title: "Signal Region Cutflow" of "Search for Majorana neutrinos in same-sign $WW$ scattering events from $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Cutflow for a selection of signal samples used in this analysis. The flavour-aligned scenario (in which $\vert V_{\mu N} \vert^{2}=1$) is considered for heavy Majorana neutrino samples. The event yields include all correction factors applied to simulation, and is normalised to 140 fb$^{-1}$. The `Skim' selection requires 2 baseline muons and 2 jets satisfying the object definitions described in Section 3 and $m_{jj} &gt; 150$ GeV. Uncertainties are statistical only.
description: A search for Majorana neutrinos in same-sign $W^{\pm}W^{\pm}$ scattering events is presented. The analysis uses the proton-proton collision data recorded by the ATLAS detector at $\sqrt{s}= 13$ TeV at the Large Hadron Collider during the years 2015-2018, corresponding to an integrated luminosity of 140 fb$^{-1}$. The analysis targets final states including exactly two same-sign muons and at least two hadronic jets well separated in rapidity. The modelling of the main backgrounds from Standard Model, same-sign $W^{\pm}W^{\pm}$ scattering and $WZ$ production, are constrained with data in dedicated signal-depleted control regions and the transverse momenta of the sub-leading muon is used to search for signals originating from a heavy Majorana neutrino with masses of 50 GeV to 20 TeV. The presence of a signal is examined in a signal-enriched region and is interpreted in a benchmark scenario of the Phenomenological Type I Seesaw model. In addition, the sensitivity to the Weinberg operator is investigated. No significant excess is observed over the background expectation. Upper limits at the 95% confidence level are provided on the squared muon heavy neutrino mixing element $\vert V_{\mu N} \vert^{2}$ as a function of the heavy Majorana neutrino mass $m_N$, and on the effective $\mu\mu$ Majorana neutrino mass $|m_{\mu\mu}|$.
DOI: 10.17182/hepdata.141495.v1/t1
title: "Figure 3(a)" of "Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Inclusive photon multiplicity distribution measured within $2.3&lt;\eta_{\rm lab}&lt;3.9$ in pp collisions at $\sqrt{s} = 5020~\mathrm{GeV}$.
description: CERN-LHC. A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$ using the ALICE detector in the forward pseudorapidity region $2.3&lt;\eta_{\rm lab}&lt;3.9$ is presented. Measurements in p-Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p-Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p-Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in pp collisions and for different centrality classes in p-Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.
DOI: 10.17182/hepdata.141495.v1/t2
title: "Figure 3(b)" of "Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Inclusive photon multiplicity distribution measured within $2.3&lt;\eta_{\rm lab}&lt;3.9$ in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$.
description: CERN-LHC. A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$ using the ALICE detector in the forward pseudorapidity region $2.3&lt;\eta_{\rm lab}&lt;3.9$ is presented. Measurements in p-Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p-Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p-Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in pp collisions and for different centrality classes in p-Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.
DOI: 10.17182/hepdata.141495.v1/t3
title: "Figure 3(c)" of "Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Inclusive photon multiplicity distribution measured within $2.3&lt;\eta_{\rm lab}&lt;3.9$ in Pb-p collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$.
description: CERN-LHC. A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$ using the ALICE detector in the forward pseudorapidity region $2.3&lt;\eta_{\rm lab}&lt;3.9$ is presented. Measurements in p-Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p-Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p-Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in pp collisions and for different centrality classes in p-Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.
DOI: 10.17182/hepdata.141495.v1/t4
title: "Figure 5(a)" of "Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Pseudorapidity distribution of inclusive photons measured within $2.3&lt;\eta_{\rm lab}&lt;3.9$ in pp collisions at $\sqrt{s} = 5020~\mathrm{GeV}$.
description: CERN-LHC. A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$ using the ALICE detector in the forward pseudorapidity region $2.3&lt;\eta_{\rm lab}&lt;3.9$ is presented. Measurements in p-Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p-Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p-Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in pp collisions and for different centrality classes in p-Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.
DOI: 10.17182/hepdata.141495.v1/t5
title: "Figure 5(b)" of "Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Pseudorapidity distribution of inclusive photons measured within $2.3&lt;\eta_{\rm lab}&lt;3.9$ in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$.
description: CERN-LHC. A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$ using the ALICE detector in the forward pseudorapidity region $2.3&lt;\eta_{\rm lab}&lt;3.9$ is presented. Measurements in p-Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p-Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p-Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in pp collisions and for different centrality classes in p-Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.
DOI: 10.17182/hepdata.141495.v1/t6
title: "Figure 5(c)" of "Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Pseudorapidity distribution of inclusive photons measured within $2.3&lt;\eta_{\rm lab}&lt;3.9$ in Pb-p collisions at $\sqrt{s_\mathrm{NN}} = 5020~\mathrm{GeV}$.
description: CERN-LHC. A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$ using the ALICE detector in the forward pseudorapidity region $2.3&lt;\eta_{\rm lab}&lt;3.9$ is presented. Measurements in p-Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p-Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p-Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in pp collisions and for different centrality classes in p-Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.
DOI: 10.17182/hepdata.141495.v1/t7
title: "Figure 6(a)" of "Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Pseudorapidity distribution of inclusive photons measured within $2.3&lt;\eta_{\rm lab}&lt;3.9$ in pp collisions at various LHC energies.
description: CERN-LHC. A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p-Pb collisions at a center-of-mass energy per nucleon-nucleon collision of $\sqrt{s_\mathrm{NN}} = 5.02~\mathrm{TeV}$ using the ALICE detector in the forward pseudorapidity region $2.3&lt;\eta_{\rm lab}&lt;3.9$ is presented. Measurements in p-Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p-Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p-Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in pp collisions and for different centrality classes in p-Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.