cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141455.v1/t43
title: "Figure 6-b, $m=1~\mathrm{TeV}$, 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=1~\mathrm{TeV}$. The exclusion limits are given up to coupling values at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, the narrow width approximation intrinsic to the search strategy is not considered valid. The enclosed regions are excluded.
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/t44
title: "Figure 6-b, $m=1~\mathrm{TeV}$, 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=1~\mathrm{TeV}$. The exclusion limits are given up to coupling values at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, the narrow width approximation intrinsic to the search strategy is not considered valid. The enclosed regions are excluded.
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/t45
title: "Figure 6-b, $m=1~\mathrm{TeV}$, $\Gamma=0.5\sigma$" 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=1~\mathrm{TeV}$. The coupling values are shown at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, 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.141455.v1/t46
title: "Figure 6-b, $m=1.5~\mathrm{TeV}$, 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=1.5~\mathrm{TeV}$. The exclusion limits are given up to coupling values at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, the narrow width approximation intrinsic to the search strategy is not considered valid. The enclosed regions are excluded.
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/t47
title: "Figure 6-b, $m=1.5~\mathrm{TeV}$, 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=1.5~\mathrm{TeV}$. The exclusion limits are given up to coupling values at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, the narrow width approximation intrinsic to the search strategy is not considered valid. The enclosed regions are excluded.
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/t48
title: "Figure 6-b, $m=1.5~\mathrm{TeV}$, $\Gamma=0.5\sigma$" 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=1.5~\mathrm{TeV}$. The coupling values are shown at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, 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.141455.v1/t49
title: "Figure 6-b, $m=2~\mathrm{TeV}$, 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=2~\mathrm{TeV}$. The exclusion limits are given up to coupling values at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, the narrow width approximation intrinsic to the search strategy is not considered valid. The enclosed regions are excluded.
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/t50
title: "Figure 6-b, $m=2~\mathrm{TeV}$, $\Gamma=0.5\sigma$" 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 $|g_{\mathrm{b}}|$--$|g_{\ell}|$ plane for the LFU model, with $|\delta_{\mathrm{bs}}|=0.25$ and $|g_{\nu}|=|g_{\ell}|$, for $m_{\mathrm{Z'}}=2~\mathrm{TeV}$. The coupling values are shown at which the $\mathrm{Z'}$ width is equal to half of the $\mu\mu$ invariant mass resolution. Beyond these coupling values, 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.141455.v1/t51
title: "Figure 7-a" 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 $|\theta_{23}|$--$|g_{\mathrm{Z'}}|$ plane for the $B_{3}\!-\!L_{2}$ model from JHEP 04 (2023) 033, for $m_{\mathrm{Z'}}=500~\mathrm{GeV}$. The solid black (dashed red) curves represent the observed (median expected) exclusions. The dotted curves denote 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 dotted curves is (expected to be) excluded. The dotted curve for $m_{\mathrm{Z'}}=500~\mathrm{GeV}$ lies beyond the displayed $|g_{\mathrm{Z'}}|$ range and is, therefore, not shown. The shaded blue area represents the region preferred from the global fit in JHEP 04 (2023) 033 at $95\%$ CL. The region above the green dash-dotted curve is incompatible at $95\%$ CL with the measurement of the mass difference between the mass eigenstates of the neutral $\mathrm{B}_\mathrm{s}$ mesons.
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/t52
title: "Figure 7-a, 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 $|\theta_{23}|$--$|g_{\mathrm{Z'}}|$ plane for the $B_{3}\!-\!L_{2}$ model from JHEP 04 (2023) 033, for $m_{\mathrm{Z'}}=500~\mathrm{GeV}$.
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/t53
title: "Figure 7-a, 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 $|\theta_{23}|$--$|g_{\mathrm{Z'}}|$ plane for the $B_{3}\!-\!L_{2}$ model from JHEP 04 (2023) 033, for $m_{\mathrm{Z'}}=500~\mathrm{GeV}$.
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