cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141453.v1/t3
title: "Figure 7c" of "Measurement of emission angle anisotropy via long-range angular correlations with high $p_T$ hadrons in $d$$+$Au and $p$$+$$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Fourier fit coefficients for CNT-MPCS (Au-going) correlations, as a function of collision system and $\pi^0$ $p_T$: Fractional systematic uncertainty on the quadrupole coefficient $c_2$ for $p$+$p$.
description: We present measurements of two-particle angular correlations between high-transverse-momentum ( 2&lt; $p_T$ &lt; 11 GeV/$c$) $\pi^0$ observed at midrapidity ($|\eta|$ &lt; 0.35) and particles produced either at forward (3.1 &lt; $\eta$ &lt; 3.9) or backward (−3.7 &lt; $\eta$ &lt; −3.1) rapidity in $d$+Au and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The azimuthal angle correlations for particle pairs with this large rapidity gap in the Au-going direction exhibit a ridge-like structure that persists up to $p_T$ ≈ 6 GeV/$c$ and which strongly depends on collision centrality, which is a similar characteristic to the hydrodynamical particle flow in A+A collisions. The ridge-like structure is absent in the $d$-going direction as well as in $p$+$p$ collisions, in the transverse-momentum range studied. The results indicate that the ridge-like structure is shifted in the Au-going direction toward more central collisions, similar to the charged-particle pseudorapidity distributions.
DOI: 10.17182/hepdata.141453.v1/t4
title: "Figure 8a" of "Measurement of emission angle anisotropy via long-range angular correlations with high $p_T$ hadrons in $d$$+$Au and $p$$+$$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Fourier fit coefficients for CNT-MPCN ($d$-going) correlations, as a function of collision system and $\pi^0$ $p_T$: (a) the negative of the dipole coefficient, $-c_1$; (b) the quadrupole coefficient $c_2$; (c) the ratio ${-c_2}/{c_1}$.
description: We present measurements of two-particle angular correlations between high-transverse-momentum ( 2&lt; $p_T$ &lt; 11 GeV/$c$) $\pi^0$ observed at midrapidity ($|\eta|$ &lt; 0.35) and particles produced either at forward (3.1 &lt; $\eta$ &lt; 3.9) or backward (−3.7 &lt; $\eta$ &lt; −3.1) rapidity in $d$+Au and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The azimuthal angle correlations for particle pairs with this large rapidity gap in the Au-going direction exhibit a ridge-like structure that persists up to $p_T$ ≈ 6 GeV/$c$ and which strongly depends on collision centrality, which is a similar characteristic to the hydrodynamical particle flow in A+A collisions. The ridge-like structure is absent in the $d$-going direction as well as in $p$+$p$ collisions, in the transverse-momentum range studied. The results indicate that the ridge-like structure is shifted in the Au-going direction toward more central collisions, similar to the charged-particle pseudorapidity distributions.
DOI: 10.17182/hepdata.141453.v1/t5
title: "Figure 8b" of "Measurement of emission angle anisotropy via long-range angular correlations with high $p_T$ hadrons in $d$$+$Au and $p$$+$$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Fourier fit coefficients for CNT-MPCN ($d$-going) correlations, as a function of collision system and $\pi^0$ $p_T$: Fractional systematic uncertainty on the quadrupole coefficient $c_2$ for $d$+Au.
description: We present measurements of two-particle angular correlations between high-transverse-momentum ( 2&lt; $p_T$ &lt; 11 GeV/$c$) $\pi^0$ observed at midrapidity ($|\eta|$ &lt; 0.35) and particles produced either at forward (3.1 &lt; $\eta$ &lt; 3.9) or backward (−3.7 &lt; $\eta$ &lt; −3.1) rapidity in $d$+Au and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The azimuthal angle correlations for particle pairs with this large rapidity gap in the Au-going direction exhibit a ridge-like structure that persists up to $p_T$ ≈ 6 GeV/$c$ and which strongly depends on collision centrality, which is a similar characteristic to the hydrodynamical particle flow in A+A collisions. The ridge-like structure is absent in the $d$-going direction as well as in $p$+$p$ collisions, in the transverse-momentum range studied. The results indicate that the ridge-like structure is shifted in the Au-going direction toward more central collisions, similar to the charged-particle pseudorapidity distributions.
DOI: 10.17182/hepdata.141453.v1/t6
title: "Figure 8c" of "Measurement of emission angle anisotropy via long-range angular correlations with high $p_T$ hadrons in $d$$+$Au and $p$$+$$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Fourier fit coefficients for CNT-MPCN ($d$-going) correlations, as a function of collision system and $\pi^0$ $p_T$: Fractional systematic uncertainty on the quadrupole coefficient $c_2$ for $d$+Au and $p$+$p$.
description: We present measurements of two-particle angular correlations between high-transverse-momentum ( 2&lt; $p_T$ &lt; 11 GeV/$c$) $\pi^0$ observed at midrapidity ($|\eta|$ &lt; 0.35) and particles produced either at forward (3.1 &lt; $\eta$ &lt; 3.9) or backward (−3.7 &lt; $\eta$ &lt; −3.1) rapidity in $d$+Au and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The azimuthal angle correlations for particle pairs with this large rapidity gap in the Au-going direction exhibit a ridge-like structure that persists up to $p_T$ ≈ 6 GeV/$c$ and which strongly depends on collision centrality, which is a similar characteristic to the hydrodynamical particle flow in A+A collisions. The ridge-like structure is absent in the $d$-going direction as well as in $p$+$p$ collisions, in the transverse-momentum range studied. The results indicate that the ridge-like structure is shifted in the Au-going direction toward more central collisions, similar to the charged-particle pseudorapidity distributions.
DOI: 10.17182/hepdata.141453.v1/t7
title: "Figure 9a" of "Measurement of emission angle anisotropy via long-range angular correlations with high $p_T$ hadrons in $d$$+$Au and $p$$+$$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: System centrality dependence of correlation coefficients $-c_1$, $c_2$, and the ratio ${-c_2}/{c_1}$ as a function of $N_{part}$.
description: We present measurements of two-particle angular correlations between high-transverse-momentum ( 2&lt; $p_T$ &lt; 11 GeV/$c$) $\pi^0$ observed at midrapidity ($|\eta|$ &lt; 0.35) and particles produced either at forward (3.1 &lt; $\eta$ &lt; 3.9) or backward (−3.7 &lt; $\eta$ &lt; −3.1) rapidity in $d$+Au and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The azimuthal angle correlations for particle pairs with this large rapidity gap in the Au-going direction exhibit a ridge-like structure that persists up to $p_T$ ≈ 6 GeV/$c$ and which strongly depends on collision centrality, which is a similar characteristic to the hydrodynamical particle flow in A+A collisions. The ridge-like structure is absent in the $d$-going direction as well as in $p$+$p$ collisions, in the transverse-momentum range studied. The results indicate that the ridge-like structure is shifted in the Au-going direction toward more central collisions, similar to the charged-particle pseudorapidity distributions.
DOI: 10.17182/hepdata.141453.v1/t8
title: "Figure 9b" of "Measurement of emission angle anisotropy via long-range angular correlations with high $p_T$ hadrons in $d$$+$Au and $p$$+$$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: System centrality dependence of correlation coefficients $-c_1$, $c_2$, and the ratio ${-c_2}/{c_1}$ as a function of $N_{part}$.
description: We present measurements of two-particle angular correlations between high-transverse-momentum ( 2&lt; $p_T$ &lt; 11 GeV/$c$) $\pi^0$ observed at midrapidity ($|\eta|$ &lt; 0.35) and particles produced either at forward (3.1 &lt; $\eta$ &lt; 3.9) or backward (−3.7 &lt; $\eta$ &lt; −3.1) rapidity in $d$+Au and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The azimuthal angle correlations for particle pairs with this large rapidity gap in the Au-going direction exhibit a ridge-like structure that persists up to $p_T$ ≈ 6 GeV/$c$ and which strongly depends on collision centrality, which is a similar characteristic to the hydrodynamical particle flow in A+A collisions. The ridge-like structure is absent in the $d$-going direction as well as in $p$+$p$ collisions, in the transverse-momentum range studied. The results indicate that the ridge-like structure is shifted in the Au-going direction toward more central collisions, similar to the charged-particle pseudorapidity distributions.
DOI: 10.17182/hepdata.141454.v1/t1
title: "Figure 3" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

description: Invariant $p_T$ spectra of the $\phi$ meson for different centrality bins in Au+Au, Cu+Cu, $d$+Au, and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of $\phi$ meson production in the $K^+K^-$ decay channel at midrapidity in $p$+$p$, $d$+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Results are presented on the $\phi$ invariant yield and the nuclear modification factor $R_{AA}$ for Au+Au and Cu+Cu, and $R_{dA}$ for $d$+Au collisions, studied as a function of transverse momentum (1 &lt; $p_T$ &lt; 7 GeV/$c$) and centrality. In central and mid-central Au+Au collisions, the $R_{AA}$ of $\phi$ exhibits a suppression relative to expectations from binary scaled $p$+$p$ results. The amount of suppression is smaller than that of the neutral pion and the $\eta$ meson in the intermediate $p_T$ range (2-5 GeV/$c$); whereas at higher $p_T$ the $\phi$, $\pi^0$, and $\eta$ show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate $p_T$ is not observed for the $\phi$ meson despite the similar mass of the proton and the $\phi$. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the $R_{AA}$ values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of $N_{part}$. The $R_{dA}$ of $\phi$ shows no evidence for cold nuclear effects within uncertainties.
DOI: 10.17182/hepdata.141454.v1/t2
title: "Figure 4" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

description: $R_{AA}$ vs. $p_T$ for $\phi$ in central Au+Au collisions, $R_{AA}$ vs. $p_T$ for $\phi$ and $\pi^0$ in 10-20% mid-central Au+Au collisions, and $R_{AA}$ vs. $p_T$ for $\phi$ and $p$+$\bar{p}$ in 60-92% and for $\pi^0$ in 80-92% peripheral Au+Au collisions. The global uncertainty of ~ 10% related to the $p$+$p$ reference normalization is not shown.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of $\phi$ meson production in the $K^+K^-$ decay channel at midrapidity in $p$+$p$, $d$+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Results are presented on the $\phi$ invariant yield and the nuclear modification factor $R_{AA}$ for Au+Au and Cu+Cu, and $R_{dA}$ for $d$+Au collisions, studied as a function of transverse momentum (1 &lt; $p_T$ &lt; 7 GeV/$c$) and centrality. In central and mid-central Au+Au collisions, the $R_{AA}$ of $\phi$ exhibits a suppression relative to expectations from binary scaled $p$+$p$ results. The amount of suppression is smaller than that of the neutral pion and the $\eta$ meson in the intermediate $p_T$ range (2-5 GeV/$c$); whereas at higher $p_T$ the $\phi$, $\pi^0$, and $\eta$ show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate $p_T$ is not observed for the $\phi$ meson despite the similar mass of the proton and the $\phi$. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the $R_{AA}$ values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of $N_{part}$. The $R_{dA}$ of $\phi$ shows no evidence for cold nuclear effects within uncertainties.
DOI: 10.17182/hepdata.141454.v1/t3
title: "Figure 5" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

description: $R_{AA}$ vs. $p_T$ for $\phi$ for 30-40% centrality Au+Au and 0-10% centrality Cu+Cu collisions, and $R_{AA}$ vs. $p_T$ for $\phi$ and $\pi^0$ for 40-50% centrality Au+Au and 10-20% centrality Cu+Cu collisions. The global uncertainty of ~ 10% related to the $p$+$p$ reference normalization is not shown.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of $\phi$ meson production in the $K^+K^-$ decay channel at midrapidity in $p$+$p$, $d$+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Results are presented on the $\phi$ invariant yield and the nuclear modification factor $R_{AA}$ for Au+Au and Cu+Cu, and $R_{dA}$ for $d$+Au collisions, studied as a function of transverse momentum (1 &lt; $p_T$ &lt; 7 GeV/$c$) and centrality. In central and mid-central Au+Au collisions, the $R_{AA}$ of $\phi$ exhibits a suppression relative to expectations from binary scaled $p$+$p$ results. The amount of suppression is smaller than that of the neutral pion and the $\eta$ meson in the intermediate $p_T$ range (2-5 GeV/$c$); whereas at higher $p_T$ the $\phi$, $\pi^0$, and $\eta$ show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate $p_T$ is not observed for the $\phi$ meson despite the similar mass of the proton and the $\phi$. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the $R_{AA}$ values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of $N_{part}$. The $R_{dA}$ of $\phi$ shows no evidence for cold nuclear effects within uncertainties.
DOI: 10.17182/hepdata.141454.v1/t4
title: "Figure 6a" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

description: $R_{AA}$ for $\phi$ integrated at $p_T$ &gt; 2.2 GeV/$c$ in Cu+Cu and Au+Au collisions vs. $N_{part}$. The global uncertainty related to the $p$+$p$ reference normalization is shown as a box on the right in the figure from the paper.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of $\phi$ meson production in the $K^+K^-$ decay channel at midrapidity in $p$+$p$, $d$+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Results are presented on the $\phi$ invariant yield and the nuclear modification factor $R_{AA}$ for Au+Au and Cu+Cu, and $R_{dA}$ for $d$+Au collisions, studied as a function of transverse momentum (1 &lt; $p_T$ &lt; 7 GeV/$c$) and centrality. In central and mid-central Au+Au collisions, the $R_{AA}$ of $\phi$ exhibits a suppression relative to expectations from binary scaled $p$+$p$ results. The amount of suppression is smaller than that of the neutral pion and the $\eta$ meson in the intermediate $p_T$ range (2-5 GeV/$c$); whereas at higher $p_T$ the $\phi$, $\pi^0$, and $\eta$ show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate $p_T$ is not observed for the $\phi$ meson despite the similar mass of the proton and the $\phi$. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the $R_{AA}$ values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of $N_{part}$. The $R_{dA}$ of $\phi$ shows no evidence for cold nuclear effects within uncertainties.
DOI: 10.17182/hepdata.141454.v1/t5
title: "Figure 6b" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

description: $R_{AA}$ for $\phi$ integrated at $p_T$ &gt; 2.2 GeV/$c$ in Cu+Cu and Au+Au collisions vs. $N_{part}$. The global uncertainty related to the $p$+$p$ reference normalization is shown as a box on the right in the figure from the paper.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of $\phi$ meson production in the $K^+K^-$ decay channel at midrapidity in $p$+$p$, $d$+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Results are presented on the $\phi$ invariant yield and the nuclear modification factor $R_{AA}$ for Au+Au and Cu+Cu, and $R_{dA}$ for $d$+Au collisions, studied as a function of transverse momentum (1 &lt; $p_T$ &lt; 7 GeV/$c$) and centrality. In central and mid-central Au+Au collisions, the $R_{AA}$ of $\phi$ exhibits a suppression relative to expectations from binary scaled $p$+$p$ results. The amount of suppression is smaller than that of the neutral pion and the $\eta$ meson in the intermediate $p_T$ range (2-5 GeV/$c$); whereas at higher $p_T$ the $\phi$, $\pi^0$, and $\eta$ show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate $p_T$ is not observed for the $\phi$ meson despite the similar mass of the proton and the $\phi$. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the $R_{AA}$ values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of $N_{part}$. The $R_{dA}$ of $\phi$ shows no evidence for cold nuclear effects within uncertainties.
DOI: 10.17182/hepdata.141454.v1/t6
title: "Figure 7" of "Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV"

description: $R_{dA}$ vs. $p_T$ for $\phi$, $\pi^0$, and ($p$+$\bar{p}$) for 0-20% centrality $d$+Au collisions, and $R_{dA}$ vs. $p_T$ for $\phi$, $\pi^0$, and ($p$+$\bar{p}$) for 60-88% peripheral $d$+Au collisions. The global uncertainty of ~ 10% related to the $p$+$p$ reference normalization is not shown.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of $\phi$ meson production in the $K^+K^-$ decay channel at midrapidity in $p$+$p$, $d$+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Results are presented on the $\phi$ invariant yield and the nuclear modification factor $R_{AA}$ for Au+Au and Cu+Cu, and $R_{dA}$ for $d$+Au collisions, studied as a function of transverse momentum (1 &lt; $p_T$ &lt; 7 GeV/$c$) and centrality. In central and mid-central Au+Au collisions, the $R_{AA}$ of $\phi$ exhibits a suppression relative to expectations from binary scaled $p$+$p$ results. The amount of suppression is smaller than that of the neutral pion and the $\eta$ meson in the intermediate $p_T$ range (2-5 GeV/$c$); whereas at higher $p_T$ the $\phi$, $\pi^0$, and $\eta$ show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate $p_T$ is not observed for the $\phi$ meson despite the similar mass of the proton and the $\phi$. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the $R_{AA}$ values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of $N_{part}$. The $R_{dA}$ of $\phi$ shows no evidence for cold nuclear effects within uncertainties.
DOI: 10.17182/hepdata.141455.v1/t1
title: "Figure 1-a" of "Search for a high-mass dimuon resonance produced in association with b quark jets at $\sqrt{s}$=13 TeV"

description: Feynman diagrams of $\mathrm{Z'}\to\mu^{-}\mu^{+}$ with a $\mathrm{Z'}$ boson produced via $\mathrm{b}\overline{\mathrm{b}}\to\mathrm{Z'}$, with one $\mathrm{b}$ quark in the final state.
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/t2
title: "Figure 1-b" of "Search for a high-mass dimuon resonance produced in association with b quark jets at $\sqrt{s}$=13 TeV"

description: Feynman diagrams of $\mathrm{Z'}\to\mu^{-}\mu^{+}$ with a $\mathrm{Z'}$ boson produced via $\mathrm{s}\overline{\mathrm{b}}\to\mathrm{Z'}$, with one $\mathrm{b}$ quark in the final state.
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