cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.80166.v1/t3
title: "Cross-section limits" of "Search for narrow and broad dijet resonances in proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter mediators and other new particles"

description: The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for quark-quark, quark-gluon, and gluon-gluon type dijet resonances.
description: Searches are presented for resonances decaying to dijet final states in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$. A low-mass search, for a resonance mass between 0.6 and 1.6 TeV, is performed using dijets reconstructed at the trigger level with calorimeter information, in a data set corresponding to an integrated luminosity of $27~\mathrm{fb}^{-1}$. A high-mass search, for resonances above 1.6 TeV, is performed using dijets reconstructed with the particle-flow algorithm in a data set corresponding to $36~\mathrm{fb}^{-1}$. The dijet mass spectrum is well described by a smooth parameterization and no significant evidence for the production of new particles is observed. Upper limits at $95\%$ confidence level are reported on the production cross section for narrow resonances with masses above 0.6 TeV. In the context of specific models, the limits exclude string resonances with masses below 7.7 TeV, scalar diquarks below 7.2 TeV, axigluons and colorons below 6.1 TeV, excited quarks below 6.0 TeV, color-octet scalars below $3.4~\mathrm{TeV}$, W$^{\prime}$ bosons below 3.3 TeV, Z$^{\prime}$ bosons below 2.7 TeV, RS gravitons below $1.7~\mathrm{TeV}$ and between 2.1 and 2.5 TeV, and dark matter mediators below 2.6 TeV. The limits on both vector and axial-vector mediators, in a simplified model of interactions between quarks and dark matter, are also presented as functions of dark matter mass and coupling to quarks. Limits are presented for resonances with intrinsic width as large as $30\%$ of the resonance mass, and are used to improve and extend the exclusions of a dark matter mediator to larger values of mass and coupling.
DOI: 10.17182/hepdata.80166.v1/t4
title: "Coupling limits (DM mediator)" of "Search for narrow and broad dijet resonances in proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter mediators and other new particles"

description: The observed and expected 95% CL upper limits on the universal quark coupling $g_{q}$ as a function of resonance mass for a vector mediator of interactions between quarks and dark matter.
description: Searches are presented for resonances decaying to dijet final states in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$. A low-mass search, for a resonance mass between 0.6 and 1.6 TeV, is performed using dijets reconstructed at the trigger level with calorimeter information, in a data set corresponding to an integrated luminosity of $27~\mathrm{fb}^{-1}$. A high-mass search, for resonances above 1.6 TeV, is performed using dijets reconstructed with the particle-flow algorithm in a data set corresponding to $36~\mathrm{fb}^{-1}$. The dijet mass spectrum is well described by a smooth parameterization and no significant evidence for the production of new particles is observed. Upper limits at $95\%$ confidence level are reported on the production cross section for narrow resonances with masses above 0.6 TeV. In the context of specific models, the limits exclude string resonances with masses below 7.7 TeV, scalar diquarks below 7.2 TeV, axigluons and colorons below 6.1 TeV, excited quarks below 6.0 TeV, color-octet scalars below $3.4~\mathrm{TeV}$, W$^{\prime}$ bosons below 3.3 TeV, Z$^{\prime}$ bosons below 2.7 TeV, RS gravitons below $1.7~\mathrm{TeV}$ and between 2.1 and 2.5 TeV, and dark matter mediators below 2.6 TeV. The limits on both vector and axial-vector mediators, in a simplified model of interactions between quarks and dark matter, are also presented as functions of dark matter mass and coupling to quarks. Limits are presented for resonances with intrinsic width as large as $30\%$ of the resonance mass, and are used to improve and extend the exclusions of a dark matter mediator to larger values of mass and coupling.
DOI: 10.17182/hepdata.80166.v1/t5
title: "Coupling limits (Quark only)" of "Search for narrow and broad dijet resonances in proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter mediators and other new particles"

description: The observed and expected 95% CL upper limits on the universal quark coupling $g_{q}'$ as a function of resonance mass for a leptophobic Z' resonance that only couples to quarks.
description: Searches are presented for resonances decaying to dijet final states in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$. A low-mass search, for a resonance mass between 0.6 and 1.6 TeV, is performed using dijets reconstructed at the trigger level with calorimeter information, in a data set corresponding to an integrated luminosity of $27~\mathrm{fb}^{-1}$. A high-mass search, for resonances above 1.6 TeV, is performed using dijets reconstructed with the particle-flow algorithm in a data set corresponding to $36~\mathrm{fb}^{-1}$. The dijet mass spectrum is well described by a smooth parameterization and no significant evidence for the production of new particles is observed. Upper limits at $95\%$ confidence level are reported on the production cross section for narrow resonances with masses above 0.6 TeV. In the context of specific models, the limits exclude string resonances with masses below 7.7 TeV, scalar diquarks below 7.2 TeV, axigluons and colorons below 6.1 TeV, excited quarks below 6.0 TeV, color-octet scalars below $3.4~\mathrm{TeV}$, W$^{\prime}$ bosons below 3.3 TeV, Z$^{\prime}$ bosons below 2.7 TeV, RS gravitons below $1.7~\mathrm{TeV}$ and between 2.1 and 2.5 TeV, and dark matter mediators below 2.6 TeV. The limits on both vector and axial-vector mediators, in a simplified model of interactions between quarks and dark matter, are also presented as functions of dark matter mass and coupling to quarks. Limits are presented for resonances with intrinsic width as large as $30\%$ of the resonance mass, and are used to improve and extend the exclusions of a dark matter mediator to larger values of mass and coupling.
DOI: 10.17182/hepdata.80167.v1/t1
title: "Table 1" of "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Unfolded distributions of particle density in Z events, as a function of $p_{T}^{\mu\mu}$ in the towards ($\Delta\phi&lt; 60^{\circ}$) region. Error bars represent the statistical and systematic uncertainties added in quadrature.
description: Measurement of the underlying event activity, in proton-proton collisions at a centre-of-mass energy of 13 TeV, performed using inclusive Z-boson events collected by the CMS experiment at the Large Hadron Collider. The analyzed data corresponds to an integrated luminosity of 2.1 fb-1. The underlying event activity is quantified in terms of charged particle multiplicity and their scalar sum of their transverse momentum in different topological regions defined with respect to the resultatnt azimuthal direction of the two muons coming from the decay of a Z-boson. The distributions are unfolded to stable charged-particle level and are compared with predictions from various simulations, as well as with the measurements at a centre-of-mass energy of 1.96 TeV and 7 TeV by the CDF and CMS experiments.
Events are selected online by requiring the presence of at least two isolated muon candidates with - $p_T &gt; 17\,(8)$ GeV for the leading (subleading) muon - Offline, the leading and subleading muons are required to have a $p_T$ larger than 20 and 10 GeV, respectively - Events with two oppositely charged muons are further required to have an invariant mass ($M_{\mu\mu}$) in the window 81--101 GeV. - All charged particles, except selected muons, with $p_T &gt; 0.5 GeV$ and $|\eta| &lt; 2 $ are considered for the UE study.
Particle density- The average number of charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
$\Sigma p_T$ density- The average of the scalar $p_T$ sum of all selected charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
DOI: 10.17182/hepdata.80167.v1/t2
title: "Table 2" of "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Unfolded distributions of particle density in Z events, as a function of $p_{T}^{\mu\mu}$ in the transverse ($60^{\circ} &lt;\Delta\phi&lt; 120^{\circ}$) region. Error bars represent the statistical and systematic uncertainties added in quadrature.
description: Measurement of the underlying event activity, in proton-proton collisions at a centre-of-mass energy of 13 TeV, performed using inclusive Z-boson events collected by the CMS experiment at the Large Hadron Collider. The analyzed data corresponds to an integrated luminosity of 2.1 fb-1. The underlying event activity is quantified in terms of charged particle multiplicity and their scalar sum of their transverse momentum in different topological regions defined with respect to the resultatnt azimuthal direction of the two muons coming from the decay of a Z-boson. The distributions are unfolded to stable charged-particle level and are compared with predictions from various simulations, as well as with the measurements at a centre-of-mass energy of 1.96 TeV and 7 TeV by the CDF and CMS experiments.
Events are selected online by requiring the presence of at least two isolated muon candidates with - $p_T &gt; 17\,(8)$ GeV for the leading (subleading) muon - Offline, the leading and subleading muons are required to have a $p_T$ larger than 20 and 10 GeV, respectively - Events with two oppositely charged muons are further required to have an invariant mass ($M_{\mu\mu}$) in the window 81--101 GeV. - All charged particles, except selected muons, with $p_T &gt; 0.5 GeV$ and $|\eta| &lt; 2 $ are considered for the UE study.
Particle density- The average number of charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
$\Sigma p_T$ density- The average of the scalar $p_T$ sum of all selected charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
DOI: 10.17182/hepdata.80167.v1/t3
title: "Table 3" of "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Unfolded distributions of particle density in Z events, as a function of $p_{T}^{\mu\mu}$ in the away ($\Delta\phi&gt; 120^{\circ}$) region. Error bars represent the statistical and systematic uncertainties added in quadrature.
description: Measurement of the underlying event activity, in proton-proton collisions at a centre-of-mass energy of 13 TeV, performed using inclusive Z-boson events collected by the CMS experiment at the Large Hadron Collider. The analyzed data corresponds to an integrated luminosity of 2.1 fb-1. The underlying event activity is quantified in terms of charged particle multiplicity and their scalar sum of their transverse momentum in different topological regions defined with respect to the resultatnt azimuthal direction of the two muons coming from the decay of a Z-boson. The distributions are unfolded to stable charged-particle level and are compared with predictions from various simulations, as well as with the measurements at a centre-of-mass energy of 1.96 TeV and 7 TeV by the CDF and CMS experiments.
Events are selected online by requiring the presence of at least two isolated muon candidates with - $p_T &gt; 17\,(8)$ GeV for the leading (subleading) muon - Offline, the leading and subleading muons are required to have a $p_T$ larger than 20 and 10 GeV, respectively - Events with two oppositely charged muons are further required to have an invariant mass ($M_{\mu\mu}$) in the window 81--101 GeV. - All charged particles, except selected muons, with $p_T &gt; 0.5 GeV$ and $|\eta| &lt; 2 $ are considered for the UE study.
Particle density- The average number of charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
$\Sigma p_T$ density- The average of the scalar $p_T$ sum of all selected charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
DOI: 10.17182/hepdata.80167.v1/t4
title: "Table 4" of "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Unfolded distributions of $\Sigma p_{T}$ density in Z events, as a function of $p_{T}^{\mu\mu}$ in the towards ($\Delta\phi&lt; 60^{\circ}$) region. Error bars represent the statistical and systematic uncertainties added in quadrature.
description: Measurement of the underlying event activity, in proton-proton collisions at a centre-of-mass energy of 13 TeV, performed using inclusive Z-boson events collected by the CMS experiment at the Large Hadron Collider. The analyzed data corresponds to an integrated luminosity of 2.1 fb-1. The underlying event activity is quantified in terms of charged particle multiplicity and their scalar sum of their transverse momentum in different topological regions defined with respect to the resultatnt azimuthal direction of the two muons coming from the decay of a Z-boson. The distributions are unfolded to stable charged-particle level and are compared with predictions from various simulations, as well as with the measurements at a centre-of-mass energy of 1.96 TeV and 7 TeV by the CDF and CMS experiments.
Events are selected online by requiring the presence of at least two isolated muon candidates with - $p_T &gt; 17\,(8)$ GeV for the leading (subleading) muon - Offline, the leading and subleading muons are required to have a $p_T$ larger than 20 and 10 GeV, respectively - Events with two oppositely charged muons are further required to have an invariant mass ($M_{\mu\mu}$) in the window 81--101 GeV. - All charged particles, except selected muons, with $p_T &gt; 0.5 GeV$ and $|\eta| &lt; 2 $ are considered for the UE study.
Particle density- The average number of charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
$\Sigma p_T$ density- The average of the scalar $p_T$ sum of all selected charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
DOI: 10.17182/hepdata.80167.v1/t5
title: "Table 5" of "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Unfolded distributions of $\Sigma p_{T}$ density in Z events, as a function of $p_{T}^{\mu\mu}$ in the transverse ($60^{\circ} &lt;\Delta\phi&lt; 120^{\circ}$) region. Error bars represent the statistical and systematic uncertainties added in quadrature.
description: Measurement of the underlying event activity, in proton-proton collisions at a centre-of-mass energy of 13 TeV, performed using inclusive Z-boson events collected by the CMS experiment at the Large Hadron Collider. The analyzed data corresponds to an integrated luminosity of 2.1 fb-1. The underlying event activity is quantified in terms of charged particle multiplicity and their scalar sum of their transverse momentum in different topological regions defined with respect to the resultatnt azimuthal direction of the two muons coming from the decay of a Z-boson. The distributions are unfolded to stable charged-particle level and are compared with predictions from various simulations, as well as with the measurements at a centre-of-mass energy of 1.96 TeV and 7 TeV by the CDF and CMS experiments.
Events are selected online by requiring the presence of at least two isolated muon candidates with - $p_T &gt; 17\,(8)$ GeV for the leading (subleading) muon - Offline, the leading and subleading muons are required to have a $p_T$ larger than 20 and 10 GeV, respectively - Events with two oppositely charged muons are further required to have an invariant mass ($M_{\mu\mu}$) in the window 81--101 GeV. - All charged particles, except selected muons, with $p_T &gt; 0.5 GeV$ and $|\eta| &lt; 2 $ are considered for the UE study.
Particle density- The average number of charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
$\Sigma p_T$ density- The average of the scalar $p_T$ sum of all selected charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
DOI: 10.17182/hepdata.80167.v1/t6
title: "Table 6" of "Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Unfolded distributions of $\Sigma p_{T}$ density in Z events, as a function of $p_{T}^{\mu\mu}$ in the away ($\Delta\phi&gt; 120^{\circ}$) region. Error bars represent the statistical and systematic uncertainties added in quadrature.
description: Measurement of the underlying event activity, in proton-proton collisions at a centre-of-mass energy of 13 TeV, performed using inclusive Z-boson events collected by the CMS experiment at the Large Hadron Collider. The analyzed data corresponds to an integrated luminosity of 2.1 fb-1. The underlying event activity is quantified in terms of charged particle multiplicity and their scalar sum of their transverse momentum in different topological regions defined with respect to the resultatnt azimuthal direction of the two muons coming from the decay of a Z-boson. The distributions are unfolded to stable charged-particle level and are compared with predictions from various simulations, as well as with the measurements at a centre-of-mass energy of 1.96 TeV and 7 TeV by the CDF and CMS experiments.
Events are selected online by requiring the presence of at least two isolated muon candidates with - $p_T &gt; 17\,(8)$ GeV for the leading (subleading) muon - Offline, the leading and subleading muons are required to have a $p_T$ larger than 20 and 10 GeV, respectively - Events with two oppositely charged muons are further required to have an invariant mass ($M_{\mu\mu}$) in the window 81--101 GeV. - All charged particles, except selected muons, with $p_T &gt; 0.5 GeV$ and $|\eta| &lt; 2 $ are considered for the UE study.
Particle density- The average number of charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
$\Sigma p_T$ density- The average of the scalar $p_T$ sum of all selected charged particles in an event per unit $\Delta\eta\Delta\phi$ area.
DOI: 10.17182/hepdata.80168.v2/t1
title: "Table 1" of "Measurement of charged pion, kaon, and proton production in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) at a centre-of-mass energy of 13 TeV.
description: CERN-LHC. Measurements of the transverse momentum spectra of
identified charged hadrons in proton-proton collisions at the centre-of-mass
energy of 13 TeV using data of integrated luminosity of about 0.1 nb-1.

The data cover the PT range 0.1-1.7 GeV with |rapidity| &lt; 1 with particle
identification using energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the
form: d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n where
C=(n-1)(n-2)/(nT(nT+(n-2)m)).

Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.80168.v2/t2
title: "Table 2" of "Measurement of charged pion, kaon, and proton production in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) at a centre-of-mass energy of 13 TeV.
description: CERN-LHC. Measurements of the transverse momentum spectra of
identified charged hadrons in proton-proton collisions at the centre-of-mass
energy of 13 TeV using data of integrated luminosity of about 0.1 nb-1.

The data cover the PT range 0.1-1.7 GeV with |rapidity| &lt; 1 with particle
identification using energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the
form: d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n where
C=(n-1)(n-2)/(nT(nT+(n-2)m)).

Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.80168.v2/t3
title: "Table 3" of "Measurement of charged pion, kaon, and proton production in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) at a centre-of-mass energy of 13 TeV for multiplicity class 1 (Nrec=0-9).
description: CERN-LHC. Measurements of the transverse momentum spectra of
identified charged hadrons in proton-proton collisions at the centre-of-mass
energy of 13 TeV using data of integrated luminosity of about 0.1 nb-1.

The data cover the PT range 0.1-1.7 GeV with |rapidity| &lt; 1 with particle
identification using energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the
form: d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n where
C=(n-1)(n-2)/(nT(nT+(n-2)m)).

Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.80168.v2/t4
title: "Table 4" of "Measurement of charged pion, kaon, and proton production in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) at a centre-of-mass energy of 13 TeV for multiplicity class 1 (Nrec=0-9).
description: CERN-LHC. Measurements of the transverse momentum spectra of
identified charged hadrons in proton-proton collisions at the centre-of-mass
energy of 13 TeV using data of integrated luminosity of about 0.1 nb-1.

The data cover the PT range 0.1-1.7 GeV with |rapidity| &lt; 1 with particle
identification using energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the
form: d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n where
C=(n-1)(n-2)/(nT(nT+(n-2)m)).

Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.80168.v2/t5
title: "Table 5" of "Measurement of charged pion, kaon, and proton production in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) at a centre-of-mass energy of 13 TeV for multiplicity class 2 (Nrec=10-19).
description: CERN-LHC. Measurements of the transverse momentum spectra of
identified charged hadrons in proton-proton collisions at the centre-of-mass
energy of 13 TeV using data of integrated luminosity of about 0.1 nb-1.

The data cover the PT range 0.1-1.7 GeV with |rapidity| &lt; 1 with particle
identification using energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the
form: d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n where
C=(n-1)(n-2)/(nT(nT+(n-2)m)).

Tables of the fitted dN/dy, n and T are given at the end of the record.
DOI: 10.17182/hepdata.80168.v2/t6
title: "Table 6" of "Measurement of charged pion, kaon, and proton production in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) at a centre-of-mass energy of 13 TeV for multiplicity class 2 (Nrec=10-19).
description: CERN-LHC. Measurements of the transverse momentum spectra of
identified charged hadrons in proton-proton collisions at the centre-of-mass
energy of 13 TeV using data of integrated luminosity of about 0.1 nb-1.

The data cover the PT range 0.1-1.7 GeV with |rapidity| &lt; 1 with particle
identification using energy loss in the silicon tracker.

Fits are made to the spectra with Tsallis-Pareto-type distributions of the
form: d2N/dydpt=(dN/dy).C.pt.(1+(mt-m)/nT)**-n where
C=(n-1)(n-2)/(nT(nT+(n-2)m)).

Tables of the fitted dN/dy, n and T are given at the end of the record.