cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.106162.v1/t10
title: "Model-independent limits for a general Jgamma resonance" of "Search for W$\gamma$ resonances in proton-proton collisions at $\sqrt{s} =$ 13 TeV using hadronic decays of Lorentz-boosted W bosons"

description: Expected and observed model-independent 95% CL upper limits on the product of the cross section, branching fraction, signal acceptance and W tagging efficiency for general Jgamma resonances.
description: A search for $W\gamma$ resonances in the mass range between 0.7 and 6.0 TeV is presented. The $W$ boson is reconstructed via its hadronic decays, with the final-state products forming a single large-radius jet, owing to a high Lorentz boost of the $W$ boson. The search is based on proton-proton collision data at $\sqrt{s} = 13 ~\text{TeV}$, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$, collected with the CMS detector at the LHC in 2016--2018. The $W\gamma$ mass spectrum is parameterized with a smoothly falling background function and examined for the presence of resonance-like signals. No significant excess above the predicted background is observed. Model-specific upper limits at 95% confidence level on the product of the cross section and branching fraction to the $W\gamma$ channel are set. Limits for narrow resonances and for resonances with an intrinsic width equal to 5% of their mass, for spin-0 and spin-1 hypotheses, range between 0.17 fb at 6.0 TeV and 55 fb at 0.7 TeV. These are the most restrictive limits to date on the existence of such resonances. In specific narrow-resonance benchmark models, heavy scalar (vector) triplet resonances with masses between 0.75 (1.15) and 1.40 (1.36) TeV are excluded for a range of model parameters. Model-independent limits on the product of the cross section, signal acceptance, and branching fraction to the $W\gamma$ channel are set for minimum $W\gamma$ mass thresholds between 1.5 and 8.0 TeV.
DOI: 10.17182/hepdata.106162.v1/t8
title: "Cross section limits for a broad vector Wgamma resonance" of "Search for W$\gamma$ resonances in proton-proton collisions at $\sqrt{s} =$ 13 TeV using hadronic decays of Lorentz-boosted W bosons"

description: Expected and observed 95% CL upper limits on the product of the cross section and branching fraction for broad vector Wgamma resonances.
description: A search for $W\gamma$ resonances in the mass range between 0.7 and 6.0 TeV is presented. The $W$ boson is reconstructed via its hadronic decays, with the final-state products forming a single large-radius jet, owing to a high Lorentz boost of the $W$ boson. The search is based on proton-proton collision data at $\sqrt{s} = 13 ~\text{TeV}$, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$, collected with the CMS detector at the LHC in 2016--2018. The $W\gamma$ mass spectrum is parameterized with a smoothly falling background function and examined for the presence of resonance-like signals. No significant excess above the predicted background is observed. Model-specific upper limits at 95% confidence level on the product of the cross section and branching fraction to the $W\gamma$ channel are set. Limits for narrow resonances and for resonances with an intrinsic width equal to 5% of their mass, for spin-0 and spin-1 hypotheses, range between 0.17 fb at 6.0 TeV and 55 fb at 0.7 TeV. These are the most restrictive limits to date on the existence of such resonances. In specific narrow-resonance benchmark models, heavy scalar (vector) triplet resonances with masses between 0.75 (1.15) and 1.40 (1.36) TeV are excluded for a range of model parameters. Model-independent limits on the product of the cross section, signal acceptance, and branching fraction to the $W\gamma$ channel are set for minimum $W\gamma$ mass thresholds between 1.5 and 8.0 TeV.
DOI: 10.17182/hepdata.106162.v1/t9
title: "Model-independent limits for a general Wgamma resonance" of "Search for W$\gamma$ resonances in proton-proton collisions at $\sqrt{s} =$ 13 TeV using hadronic decays of Lorentz-boosted W bosons"

description: Expected and observed model-independent 95% CL upper limits on the product of the cross section, branching fraction and signal acceptance for general Wgamma resonances.
description: A search for $W\gamma$ resonances in the mass range between 0.7 and 6.0 TeV is presented. The $W$ boson is reconstructed via its hadronic decays, with the final-state products forming a single large-radius jet, owing to a high Lorentz boost of the $W$ boson. The search is based on proton-proton collision data at $\sqrt{s} = 13 ~\text{TeV}$, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$, collected with the CMS detector at the LHC in 2016--2018. The $W\gamma$ mass spectrum is parameterized with a smoothly falling background function and examined for the presence of resonance-like signals. No significant excess above the predicted background is observed. Model-specific upper limits at 95% confidence level on the product of the cross section and branching fraction to the $W\gamma$ channel are set. Limits for narrow resonances and for resonances with an intrinsic width equal to 5% of their mass, for spin-0 and spin-1 hypotheses, range between 0.17 fb at 6.0 TeV and 55 fb at 0.7 TeV. These are the most restrictive limits to date on the existence of such resonances. In specific narrow-resonance benchmark models, heavy scalar (vector) triplet resonances with masses between 0.75 (1.15) and 1.40 (1.36) TeV are excluded for a range of model parameters. Model-independent limits on the product of the cross section, signal acceptance, and branching fraction to the $W\gamma$ channel are set for minimum $W\gamma$ mass thresholds between 1.5 and 8.0 TeV.
DOI: 10.17182/hepdata.106205.v1/t1
title: "DN/DETARAP" of "Pseudorapidity distributions of charged particles as a function of mid and forward rapidity mutiplicities in pp collisions at $\sqrt{s}$ = 5.02, 7 and 13 TeV"

description: Charged-particle pseudorapidity density for forward multiplicity classes as a function of $\eta$ in pp collisions at $\sqrt{s} = 5.02\,\mathrm{TeV}$. Statistical errors are generally insignificant.
description: CERN-LHC. The multiplicity dependence of the pseudorapidity density of charged particles in proton--proton (pp) collisions at centre-of-mass energies $\sqrt{s}$ = 5.02, 7 and 13 TeV measured by ALICE is reported. The analysis relies on track segments measured in the midrapidity range ($|\eta| &lt; 1.5$). Results are presented for inelastic events having at least one charged particle produced in the pseudorapidity interval $|\eta|&lt;1$ ($\mathrm{INEL}_{&gt;0}$). The multiplicity dependence of the pseudorapidy density of charged particles is measured with mid and forward rapidity multiplicity estimators, the latter being less affected by autocorrelations. A detailed comparison with predictions from the PYTHIA 8 and EPOS LHC event generators is also presented. Both generators provide a good description of the data.
DOI: 10.17182/hepdata.106205.v1/t2
title: "DN/DETARAP2" of "Pseudorapidity distributions of charged particles as a function of mid and forward rapidity mutiplicities in pp collisions at $\sqrt{s}$ = 5.02, 7 and 13 TeV"

description: Charged-particle pseudorapidity density for forward multiplicity classes as a function of $\eta$ in pp collisions at $\sqrt{s} = 7\,\mathrm{TeV}$. Statistical errors are generally insignificant.
description: CERN-LHC. The multiplicity dependence of the pseudorapidity density of charged particles in proton--proton (pp) collisions at centre-of-mass energies $\sqrt{s}$ = 5.02, 7 and 13 TeV measured by ALICE is reported. The analysis relies on track segments measured in the midrapidity range ($|\eta| &lt; 1.5$). Results are presented for inelastic events having at least one charged particle produced in the pseudorapidity interval $|\eta|&lt;1$ ($\mathrm{INEL}_{&gt;0}$). The multiplicity dependence of the pseudorapidy density of charged particles is measured with mid and forward rapidity multiplicity estimators, the latter being less affected by autocorrelations. A detailed comparison with predictions from the PYTHIA 8 and EPOS LHC event generators is also presented. Both generators provide a good description of the data.
DOI: 10.25549/vercoutere-ouc110610966
title: Nag's Long Jump photo

description: Photo from magazine accompanying story on "Old Nag's Long Jump from Plow" by Philip Kunhardt, Life 47(19):66; 1959-11-09. Provided by OT as inspiration for painting. See 179~01.
DOI: 10.17182/hepdata.106205.v1/t3
title: "DN/DETARAP3" of "Pseudorapidity distributions of charged particles as a function of mid and forward rapidity mutiplicities in pp collisions at $\sqrt{s}$ = 5.02, 7 and 13 TeV"

description: Charged-particle pseudorapidity density for forward multiplicity classes as a function of $\eta$ in pp collisions at $\sqrt{s} = 13\,\mathrm{TeV}$. Statistical errors are generally insignificant.
description: CERN-LHC. The multiplicity dependence of the pseudorapidity density of charged particles in proton--proton (pp) collisions at centre-of-mass energies $\sqrt{s}$ = 5.02, 7 and 13 TeV measured by ALICE is reported. The analysis relies on track segments measured in the midrapidity range ($|\eta| &lt; 1.5$). Results are presented for inelastic events having at least one charged particle produced in the pseudorapidity interval $|\eta|&lt;1$ ($\mathrm{INEL}_{&gt;0}$). The multiplicity dependence of the pseudorapidy density of charged particles is measured with mid and forward rapidity multiplicity estimators, the latter being less affected by autocorrelations. A detailed comparison with predictions from the PYTHIA 8 and EPOS LHC event generators is also presented. Both generators provide a good description of the data.
DOI: 10.17182/hepdata.106205.v1/t4
title: "DN/DETARAP4" of "Pseudorapidity distributions of charged particles as a function of mid and forward rapidity mutiplicities in pp collisions at $\sqrt{s}$ = 5.02, 7 and 13 TeV"

description: Charged-particle pseudorapidity density for central multiplicity classes as a function of $\eta$ in pp collisions at $\sqrt{s} = 5.02\,\mathrm{TeV}$. Statistical errors are generally insignificant.
description: CERN-LHC. The multiplicity dependence of the pseudorapidity density of charged particles in proton--proton (pp) collisions at centre-of-mass energies $\sqrt{s}$ = 5.02, 7 and 13 TeV measured by ALICE is reported. The analysis relies on track segments measured in the midrapidity range ($|\eta| &lt; 1.5$). Results are presented for inelastic events having at least one charged particle produced in the pseudorapidity interval $|\eta|&lt;1$ ($\mathrm{INEL}_{&gt;0}$). The multiplicity dependence of the pseudorapidy density of charged particles is measured with mid and forward rapidity multiplicity estimators, the latter being less affected by autocorrelations. A detailed comparison with predictions from the PYTHIA 8 and EPOS LHC event generators is also presented. Both generators provide a good description of the data.
DOI: 10.17182/hepdata.106205.v1/t5
title: "DN/DETARAP5" of "Pseudorapidity distributions of charged particles as a function of mid and forward rapidity mutiplicities in pp collisions at $\sqrt{s}$ = 5.02, 7 and 13 TeV"

description: Charged-particle pseudorapidity density for central multiplicity classes as a function of $\eta$ in pp collisions at $\sqrt{s} = 7\,\mathrm{TeV}$. Statistical errors are generally insignificant.
description: CERN-LHC. The multiplicity dependence of the pseudorapidity density of charged particles in proton--proton (pp) collisions at centre-of-mass energies $\sqrt{s}$ = 5.02, 7 and 13 TeV measured by ALICE is reported. The analysis relies on track segments measured in the midrapidity range ($|\eta| &lt; 1.5$). Results are presented for inelastic events having at least one charged particle produced in the pseudorapidity interval $|\eta|&lt;1$ ($\mathrm{INEL}_{&gt;0}$). The multiplicity dependence of the pseudorapidy density of charged particles is measured with mid and forward rapidity multiplicity estimators, the latter being less affected by autocorrelations. A detailed comparison with predictions from the PYTHIA 8 and EPOS LHC event generators is also presented. Both generators provide a good description of the data.
DOI: 10.17182/hepdata.106205.v1/t6
title: "DN/DETARAP6" of "Pseudorapidity distributions of charged particles as a function of mid and forward rapidity mutiplicities in pp collisions at $\sqrt{s}$ = 5.02, 7 and 13 TeV"

description: Charged-particle pseudorapidity density for central multiplicity classes as a function of $\eta$ in pp collisions at $\sqrt{s} = 13\,\mathrm{TeV}$. Statistical errors are generally insignificant.
description: CERN-LHC. The multiplicity dependence of the pseudorapidity density of charged particles in proton--proton (pp) collisions at centre-of-mass energies $\sqrt{s}$ = 5.02, 7 and 13 TeV measured by ALICE is reported. The analysis relies on track segments measured in the midrapidity range ($|\eta| &lt; 1.5$). Results are presented for inelastic events having at least one charged particle produced in the pseudorapidity interval $|\eta|&lt;1$ ($\mathrm{INEL}_{&gt;0}$). The multiplicity dependence of the pseudorapidy density of charged particles is measured with mid and forward rapidity multiplicity estimators, the latter being less affected by autocorrelations. A detailed comparison with predictions from the PYTHIA 8 and EPOS LHC event generators is also presented. Both generators provide a good description of the data.
DOI: 10.17182/hepdata.106472.v1/t1
title: "Figure 2-1" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 0% to 5% centrality $Au+Au$. 90% Limit on 18-20 and 20-22 GeV/c bins.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t2
title: "Figure 2-2" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 0% to 10% centrality $Au+Au$. 90% Limit on 18-20 and 20-22 GeV/c bins.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t3
title: "Figure 2-3" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 10% to 20% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t4
title: "Figure 2-4" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 0% to 20% centrality $Au+Au$. 90% Limit on 18-20 and 20-22 GeV/c bins.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t5
title: "Figure 2-5" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 20% to 40% centrality $Au+Au$. 90% Limit for 20-22 GeV/c bin.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t6
title: "Figure 2-6" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 40% to 60% centrality $Au+Au$. 90% Limit for 18-20 GeV/c bin.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t7
title: "Figure 2-7" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 20% to 60% centrality $Au+Au$. 90% Limit for 18-20 GeV/c bin.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t8
title: "Figure 2-8" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 60% to 92% centrality $Au+Au$. 90% Limit for 18-20 GeV/c bin.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.25549/vercoutere-ouc110609881
title: Family picnic in the country

description: Family picnic in the country: a female in a brown-checked blouse and a man with purple shirt sitting at a picnic table with glasses and a picnic basket; a male in a blue shirt and female in a pink dress sitting on a yellow field playing with a boy in orange and black shirt with brown pants and a red-headed girl in blue dress; a split wood fence, leafy tree, purple and brown mountains, and a blue sky in the background