cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95433.v1/t3
title: "Table 3" of "Evidence for electroweak production of four charged leptons and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Data from paper Table 3. Measured and expected fiducial cross-sections in the VBS-enriched tight fiducial region.
description: CERN LHC. A search for the electroweak (EW) production of two Z bosons in association with 2 jets (j) and constraints on anomalous quartic gauge couplings are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector in 2016-2018 and corresponding to an integrated luminosity of 137.1 fb−1. The search is performed in the fully leptonic final state where the two Z bosons decay to either a pair of electrons or a pair of muons. 
 The inclusive fiducial region is defined as: 
 pt(l) &gt; 20,10,5,5 GeV, |eta(l)|&lt; 2.5 
 60 &lt; m(ll)&lt; 120 GeV, m(4l)&gt;180 GeV 
 pT(j) &gt; 30 GeV, |eta(j)| &lt; 4.7 
 m(jj) &gt; 100 GeV and DeltaR(l,j)&gt;0.4. 
 The VBS-enriched loose selection additionally requires: 
 m(jj) &gt; 400 GeV and DeltaEta(jj)&gt;2.4. 
 The VBS-enriched tight selection additionally requires: 
 m(jj) &gt; 1 TeV and DeltaEta(jj)&gt;2.4.
DOI: 10.17182/hepdata.95433.v1/t4
title: "Table 4" of "Evidence for electroweak production of four charged leptons and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Data from paper Table 4. Observed and expected exclusion limits for the aQGC parameters at 95% CL, without any form factors.
description: CERN LHC. A search for the electroweak (EW) production of two Z bosons in association with 2 jets (j) and constraints on anomalous quartic gauge couplings are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector in 2016-2018 and corresponding to an integrated luminosity of 137.1 fb−1. The search is performed in the fully leptonic final state where the two Z bosons decay to either a pair of electrons or a pair of muons. 
 The inclusive fiducial region is defined as: 
 pt(l) &gt; 20,10,5,5 GeV, |eta(l)|&lt; 2.5 
 60 &lt; m(ll)&lt; 120 GeV, m(4l)&gt;180 GeV 
 pT(j) &gt; 30 GeV, |eta(j)| &lt; 4.7 
 m(jj) &gt; 100 GeV and DeltaR(l,j)&gt;0.4. 
 The VBS-enriched loose selection additionally requires: 
 m(jj) &gt; 400 GeV and DeltaEta(jj)&gt;2.4. 
 The VBS-enriched tight selection additionally requires: 
 m(jj) &gt; 1 TeV and DeltaEta(jj)&gt;2.4.
DOI: 10.17182/hepdata.95433.v1/t5
title: "Table 5" of "Evidence for electroweak production of four charged leptons and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Data from paper Fig.4. Observed four lepton invariant mass distribution. The last bin includes overflow.
description: CERN LHC. A search for the electroweak (EW) production of two Z bosons in association with 2 jets (j) and constraints on anomalous quartic gauge couplings are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector in 2016-2018 and corresponding to an integrated luminosity of 137.1 fb−1. The search is performed in the fully leptonic final state where the two Z bosons decay to either a pair of electrons or a pair of muons. 
 The inclusive fiducial region is defined as: 
 pt(l) &gt; 20,10,5,5 GeV, |eta(l)|&lt; 2.5 
 60 &lt; m(ll)&lt; 120 GeV, m(4l)&gt;180 GeV 
 pT(j) &gt; 30 GeV, |eta(j)| &lt; 4.7 
 m(jj) &gt; 100 GeV and DeltaR(l,j)&gt;0.4. 
 The VBS-enriched loose selection additionally requires: 
 m(jj) &gt; 400 GeV and DeltaEta(jj)&gt;2.4. 
 The VBS-enriched tight selection additionally requires: 
 m(jj) &gt; 1 TeV and DeltaEta(jj)&gt;2.4.
DOI: 10.17182/hepdata.95469.v1/t1
title: "Forward-backward asymmetry" of "Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Linearized top quark forward-backward production asymmetry $A_{FB}^{(1)}$
description: CERN-LHC-CMS. Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at sqrt(s)=13 TeV.
DOI: 10.17182/hepdata.95469.v1/t2
title: "Anomalous chromomagnetic dipole moment" of "Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Top quark anomalous chromomagnetic dipole moment $\hat{\mu}_{t}$
description: CERN-LHC-CMS. Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at sqrt(s)=13 TeV.
DOI: 10.17182/hepdata.95469.v1/t3
title: "Anomalous chromoelectric dipole moment" of "Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Top quark anomalous chromoelectric dipole moment $\hat{d}_{t}$
description: CERN-LHC-CMS. Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at sqrt(s)=13 TeV.
DOI: 10.17182/hepdata.95537.v1/t1
title: "Figure 2" of "Underlying event measurements in $p$+$p$ collisions at $\sqrt{s}= 200 $ GeV at RHIC"

description: Average charged particle multiplicity densities for Toward, Away, and Transverse regions as functions of the leading jet pT, with charged particle pT&gt;0.2 GeV/c. The wide curves are PYTHIA 6 (STAR). The middle width curves are default PYTHIA 6 Perugia 2012 tune. The thin curves are PYTHIA 8 Monash 2013 tune. The solid curves are the Toward region. The sparse dashed curves are the Away region. The dense dashed curves are the Transverse region.
description: Particle production sensitive to nonfactorizable and nonperturbative processes that contribute to the underlying event associated with a high transverse momentum (pT) jet in proton+proton collisions at sqrt(s)=200 GeV is studied with the STAR detector. Each event is divided into three regions based on the azimuthal angle with respect to the highest-pT jet direction: in the leading jet direction ("Toward"), opposite to the leading jet ("Away"), and perpendicular to the leading jet ("Transverse"). In the Transverse region, the average charged particle density is found to be between 0.4 and 0.6 and the mean transverse momentum, , between 0.5 and 0.7 GeV/c for particles with pT &gt;0.2 GeV/c at mid-pseudorapidity (|eta|&lt;1) and jet pT &gt;15 GeV/c. Both average particle density and depend weakly on the leading jet pT. Closer inspection of the Transverse region hints that contributions to the underlying event from initial- and final-state radiation are significantly smaller in these collisions than at the higher energies, up to 13 TeV, recorded at the LHC. Underlying event measurements associated with a high-pT jet will contribute to our understanding of QCD processes at hard and soft scales at RHIC energies, as well as provide constraints to modeling of underlying event dynamics.
DOI: 10.17182/hepdata.95537.v1/t2
title: "Figure 3" of "Underlying event measurements in $p$+$p$ collisions at $\sqrt{s}= 200 $ GeV at RHIC"

description: Transverse region average charged particle densities for pT&gt;0.2 GeV/c (open symbols) and pT&gt;0.5 GeV/c (filled symbols). Simulations are also shown as curves. The wide curves are PYTHIA 6 (STAR). The middle width curves are default PYTHIA 6 Perugia 2012 tune. The thin curves are PYTHIA 8 Monash 2013 tune.
description: Particle production sensitive to nonfactorizable and nonperturbative processes that contribute to the underlying event associated with a high transverse momentum (pT) jet in proton+proton collisions at sqrt(s)=200 GeV is studied with the STAR detector. Each event is divided into three regions based on the azimuthal angle with respect to the highest-pT jet direction: in the leading jet direction ("Toward"), opposite to the leading jet ("Away"), and perpendicular to the leading jet ("Transverse"). In the Transverse region, the average charged particle density is found to be between 0.4 and 0.6 and the mean transverse momentum, , between 0.5 and 0.7 GeV/c for particles with pT &gt;0.2 GeV/c at mid-pseudorapidity (|eta|&lt;1) and jet pT &gt;15 GeV/c. Both average particle density and depend weakly on the leading jet pT. Closer inspection of the Transverse region hints that contributions to the underlying event from initial- and final-state radiation are significantly smaller in these collisions than at the higher energies, up to 13 TeV, recorded at the LHC. Underlying event measurements associated with a high-pT jet will contribute to our understanding of QCD processes at hard and soft scales at RHIC energies, as well as provide constraints to modeling of underlying event dynamics.
DOI: 10.17182/hepdata.95537.v1/t3
title: "Figure 4" of "Underlying event measurements in $p$+$p$ collisions at $\sqrt{s}= 200 $ GeV at RHIC"

description: Charged particle for Toward, Away, and Transverse regions as functions of the leading jet pT, with charged particle pT&gt;0.2 GeV/c. Simulations are also shown as curves. The wide curves are PYTHIA 6 (STAR). The middle width curves are default PYTHIA 6 Perugia 2012 tune. The thin curves are PYTHIA 8 Monash 2013 tune. Note the three curves overlap for the Transverse region calculations.
description: Particle production sensitive to nonfactorizable and nonperturbative processes that contribute to the underlying event associated with a high transverse momentum (pT) jet in proton+proton collisions at sqrt(s)=200 GeV is studied with the STAR detector. Each event is divided into three regions based on the azimuthal angle with respect to the highest-pT jet direction: in the leading jet direction ("Toward"), opposite to the leading jet ("Away"), and perpendicular to the leading jet ("Transverse"). In the Transverse region, the average charged particle density is found to be between 0.4 and 0.6 and the mean transverse momentum, , between 0.5 and 0.7 GeV/c for particles with pT &gt;0.2 GeV/c at mid-pseudorapidity (|eta|&lt;1) and jet pT &gt;15 GeV/c. Both average particle density and depend weakly on the leading jet pT. Closer inspection of the Transverse region hints that contributions to the underlying event from initial- and final-state radiation are significantly smaller in these collisions than at the higher energies, up to 13 TeV, recorded at the LHC. Underlying event measurements associated with a high-pT jet will contribute to our understanding of QCD processes at hard and soft scales at RHIC energies, as well as provide constraints to modeling of underlying event dynamics.
DOI: 10.17182/hepdata.95537.v1/t4
title: "Figure 5" of "Underlying event measurements in $p$+$p$ collisions at $\sqrt{s}= 200 $ GeV at RHIC"

description: Transverse region charged particle as a function of the leading jet pT for pT&gt;0.2 GeV/c (open symbols) and pT&gt;0.5 GeV/c (filled symbols). Simulations are also shown as curves. The wide curves are PYTHIA 6 (STAR). The middle width curves are default PYTHIA 6 Perugia 2012 tune. The thin curves are PYTHIA 8 Monash 2013 tune.
description: Particle production sensitive to nonfactorizable and nonperturbative processes that contribute to the underlying event associated with a high transverse momentum (pT) jet in proton+proton collisions at sqrt(s)=200 GeV is studied with the STAR detector. Each event is divided into three regions based on the azimuthal angle with respect to the highest-pT jet direction: in the leading jet direction ("Toward"), opposite to the leading jet ("Away"), and perpendicular to the leading jet ("Transverse"). In the Transverse region, the average charged particle density is found to be between 0.4 and 0.6 and the mean transverse momentum, , between 0.5 and 0.7 GeV/c for particles with pT &gt;0.2 GeV/c at mid-pseudorapidity (|eta|&lt;1) and jet pT &gt;15 GeV/c. Both average particle density and depend weakly on the leading jet pT. Closer inspection of the Transverse region hints that contributions to the underlying event from initial- and final-state radiation are significantly smaller in these collisions than at the higher energies, up to 13 TeV, recorded at the LHC. Underlying event measurements associated with a high-pT jet will contribute to our understanding of QCD processes at hard and soft scales at RHIC energies, as well as provide constraints to modeling of underlying event dynamics.
DOI: 10.17182/hepdata.95537.v1/t5
title: "Figure 6" of "Underlying event measurements in $p$+$p$ collisions at $\sqrt{s}= 200 $ GeV at RHIC"

description: Detector-level average charged particle multiplicity densities for TransMax and TransMin as functions of the leading jet pT. Points are measured data. Histograms are calculated values assuming TransMax and TransMin are derived from the same parent distribution.
description: Particle production sensitive to nonfactorizable and nonperturbative processes that contribute to the underlying event associated with a high transverse momentum (pT) jet in proton+proton collisions at sqrt(s)=200 GeV is studied with the STAR detector. Each event is divided into three regions based on the azimuthal angle with respect to the highest-pT jet direction: in the leading jet direction ("Toward"), opposite to the leading jet ("Away"), and perpendicular to the leading jet ("Transverse"). In the Transverse region, the average charged particle density is found to be between 0.4 and 0.6 and the mean transverse momentum, , between 0.5 and 0.7 GeV/c for particles with pT &gt;0.2 GeV/c at mid-pseudorapidity (|eta|&lt;1) and jet pT &gt;15 GeV/c. Both average particle density and depend weakly on the leading jet pT. Closer inspection of the Transverse region hints that contributions to the underlying event from initial- and final-state radiation are significantly smaller in these collisions than at the higher energies, up to 13 TeV, recorded at the LHC. Underlying event measurements associated with a high-pT jet will contribute to our understanding of QCD processes at hard and soft scales at RHIC energies, as well as provide constraints to modeling of underlying event dynamics.
DOI: 10.17182/hepdata.95537.v1/t6
title: "Figure 7" of "Underlying event measurements in $p$+$p$ collisions at $\sqrt{s}= 200 $ GeV at RHIC"

description: Transverse charged particle densities at various center-of-mass collision energies. Uncertainties smaller than the marker sizes.
description: Particle production sensitive to nonfactorizable and nonperturbative processes that contribute to the underlying event associated with a high transverse momentum (pT) jet in proton+proton collisions at sqrt(s)=200 GeV is studied with the STAR detector. Each event is divided into three regions based on the azimuthal angle with respect to the highest-pT jet direction: in the leading jet direction ("Toward"), opposite to the leading jet ("Away"), and perpendicular to the leading jet ("Transverse"). In the Transverse region, the average charged particle density is found to be between 0.4 and 0.6 and the mean transverse momentum, , between 0.5 and 0.7 GeV/c for particles with pT &gt;0.2 GeV/c at mid-pseudorapidity (|eta|&lt;1) and jet pT &gt;15 GeV/c. Both average particle density and depend weakly on the leading jet pT. Closer inspection of the Transverse region hints that contributions to the underlying event from initial- and final-state radiation are significantly smaller in these collisions than at the higher energies, up to 13 TeV, recorded at the LHC. Underlying event measurements associated with a high-pT jet will contribute to our understanding of QCD processes at hard and soft scales at RHIC energies, as well as provide constraints to modeling of underlying event dynamics.
DOI: 10.17182/hepdata.95538.v1/t1
title: "Table 1" of "Search for heavy resonances decaying into a photon and a hadronically decaying Higgs boson in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Data distribution of the reconstructed $m_{J\gamma}$ and background only fitting in the single-b-tagged category. Background and signal fit functions are provided in Table 3. Background event yields are calculated using the fitted background function.
description: This Letter presents a search for the production of new heavy resonances decaying into a Higgs boson and a photon using proton-proton collision data at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $139\,\mbox{fb}^{-1}$. The analysis is performed by reconstructing hadronically decaying Higgs boson $(H\to b\bar{b})$ candidates as single large-radius jets. A novel algorithm using information about the jet constituents in the center-of-mass frame of the jet is implemented to identify the two $b$-quarks in the single jet. No significant excess of events is observed above the expected background.
DOI: 10.17182/hepdata.95538.v1/t2
title: "Table 2" of "Search for heavy resonances decaying into a photon and a hadronically decaying Higgs boson in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Data distribution of the reconstructed $m_{J\gamma}$ and background only fitting in the double-b-tagged category. Background and signal fit functions are provided in Table 3. Background event yields are calculated using the fitted background function.
description: This Letter presents a search for the production of new heavy resonances decaying into a Higgs boson and a photon using proton-proton collision data at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $139\,\mbox{fb}^{-1}$. The analysis is performed by reconstructing hadronically decaying Higgs boson $(H\to b\bar{b})$ candidates as single large-radius jets. A novel algorithm using information about the jet constituents in the center-of-mass frame of the jet is implemented to identify the two $b$-quarks in the single jet. No significant excess of events is observed above the expected background.
DOI: 10.17182/hepdata.95538.v1/t3
title: "Table 3" of "Search for heavy resonances decaying into a photon and a hadronically decaying Higgs boson in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Background and signal functions, with their fit parameters. For the background function, the parameters are fitted from the data distribution. The "Yield" is the total number of events in data in the single-b-tagged or double-b-tagged fitting range. For the single-b-tagged category, the fitting range is [1400GeV, 4200GeV], and for the double-b-tagged category, it is [600GeV, 4200GeV]. The background event yields per bin in Table 1 and Table 2 are calculated using the data yield multiplied by the integral of the normalized background function in that bin. For the signal function, the value for the parameters are from parametrisation studies and CB stands for a Crystal-Ball function. Signal distributions in Figure 1a and Figure 1b are normalized to an arbitrary yield, for illustration purpose.
description: This Letter presents a search for the production of new heavy resonances decaying into a Higgs boson and a photon using proton-proton collision data at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $139\,\mbox{fb}^{-1}$. The analysis is performed by reconstructing hadronically decaying Higgs boson $(H\to b\bar{b})$ candidates as single large-radius jets. A novel algorithm using information about the jet constituents in the center-of-mass frame of the jet is implemented to identify the two $b$-quarks in the single jet. No significant excess of events is observed above the expected background.
DOI: 10.17182/hepdata.95538.v1/t4
title: "Table 4" of "Search for heavy resonances decaying into a photon and a hadronically decaying Higgs boson in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed and expected 95% confidence-level limits on sigma x BR as a function of mZ`.
description: This Letter presents a search for the production of new heavy resonances decaying into a Higgs boson and a photon using proton-proton collision data at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $139\,\mbox{fb}^{-1}$. The analysis is performed by reconstructing hadronically decaying Higgs boson $(H\to b\bar{b})$ candidates as single large-radius jets. A novel algorithm using information about the jet constituents in the center-of-mass frame of the jet is implemented to identify the two $b$-quarks in the single jet. No significant excess of events is observed above the expected background.
DOI: 10.17182/hepdata.95538.v1/t5
title: "Table 5" of "Search for heavy resonances decaying into a photon and a hadronically decaying Higgs boson in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Cutflow Table for 1 TeV, 2 TeV, 4 TeV MC signal samples and Data. Cut0: $\mathcal{L} \times \sigma \times B(Z`\to H\gamma)\times B(H \to b\bar{b})$; Cut1: Preselection; Cut2: Photon requirement; Cut3: Large-$R$ jet requirement; Cut4: Large-$R$ jet mass optimization; Cut5: Double $b$-tagged; Cut5.1: $p_T$ optimization(Double $b$-tagged); Cut6: Single $b$-tagged; Cut6.1: $p_T$ optimization(Single $b$-tagged).
description: This Letter presents a search for the production of new heavy resonances decaying into a Higgs boson and a photon using proton-proton collision data at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $139\,\mbox{fb}^{-1}$. The analysis is performed by reconstructing hadronically decaying Higgs boson $(H\to b\bar{b})$ candidates as single large-radius jets. A novel algorithm using information about the jet constituents in the center-of-mass frame of the jet is implemented to identify the two $b$-quarks in the single jet. No significant excess of events is observed above the expected background.
DOI: 10.17182/hepdata.95543.v1/t1
title: "Figure 10.0.0.0" of "Measurement of inclusive J/$\psi$ polarization in p+p collisions at $\sqrt{s}$ = 200 GeV by the STAR experiment"

description: The J/PSI(1S) polarization parameter $\lambda_\theta$ as a function of pT measured through dielectron channel in the HX frame.
description: We report on new measurements of inclusive J/PSI(1S) polarization at mid-rapidity in p+p collisions at $\sqrts\$ = 200 GeV by the STAR experiment at RHIC. The polarization parameters, $\lambda_\theta$, $\lambda_\phi$, and $\lambda_\theta\phi$, are measured as a function of transverse momentum (pT) in both the Helicity and Collins-Soper (CS) reference frames within pT &lt; 10 GeV/c. Except for $\lambda_\theta$ in the CS frame at the highest measured pT, all three polarization parameters are consistent with 0 in both reference frames without any strong pT dependence. Several model calculations are compared with data, and the one using the Color Glass Condensate effective field theory coupled with non-relativistic QCD gives the best overall description of the experimental results, even though other models cannot be ruled out due to experimental uncertainties.