cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.25549/vercoutere-ouc110611085
title: Feathered figure surrounded by objects; Trolly and car in a street scene

description: This collection includes over 900 pieces of art that were created by patients at the Atascadero State Hospital (ASH) in the mid-1950’s.  The artists were under the treatment of Albert R. Vercoutere who used the technique of providing photos from magazines for the patients to use as inspiration for their own artwork. Although not trained in the use of art therapy and during a time when art therapy was a new approach, Vercoutere often utilized art as a mechanism for working with his patients. The artwork was created during a time when psychotropic drugs were not yet available as treatment options for mental health patients.
DOI: 10.17182/hepdata.106658.v1/t10
title: "Figure 14 fwd" of "Nuclear-modification factor of charged hadrons at forward and backward rapidity in $p$$+$Al and $p$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: RpA of charged hadrons as a function of Npart at forward and backward rapidity in p+Al collisions.
description: BNL-RHIC. The PHENIX experiment has studied nuclear effects in p+Al and p+Au collisions at $\sqrt{s_{_{NN}}}=200~{\rm GeV}$ on charged hadron production at forward rapidity ($1.4&lt;\eta&lt;2.4$, p-going direction) and backward rapidity ($-2.2&lt;\eta&lt;-1.4$, A-going direction). Such effects are quantified by measuring nuclear modification factors as a function of transverse momentum and pesudorapidity in various collision multiplicity selections. In central p+Al and p+Au collisions, a suppression (enhancement) is observed at forward (backward) rapidity compared to the binary scaled yields in p+p collisions. The magnitude of enhancement at backward rapidity is larger in p+Au collisions than in p+Al collisions, which have a smaller number of participating nucleons. However, the results at forward rapidity show a similar suppression within uncertainties. The results in the integrated centrality are compared with calculations using nuclear parton distribution functions, which show a reasonable agreement at the forward rapidity but fail to describe the backward rapidity enhancement.
DOI: 10.17182/hepdata.106658.v1/t11
title: "Figure 14 bwd" of "Nuclear-modification factor of charged hadrons at forward and backward rapidity in $p$$+$Al and $p$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: RpA of charged hadrons as a function of Npart at forward and backward rapidity in p+Au collisions.
description: BNL-RHIC. The PHENIX experiment has studied nuclear effects in p+Al and p+Au collisions at $\sqrt{s_{_{NN}}}=200~{\rm GeV}$ on charged hadron production at forward rapidity ($1.4&lt;\eta&lt;2.4$, p-going direction) and backward rapidity ($-2.2&lt;\eta&lt;-1.4$, A-going direction). Such effects are quantified by measuring nuclear modification factors as a function of transverse momentum and pesudorapidity in various collision multiplicity selections. In central p+Al and p+Au collisions, a suppression (enhancement) is observed at forward (backward) rapidity compared to the binary scaled yields in p+p collisions. The magnitude of enhancement at backward rapidity is larger in p+Au collisions than in p+Al collisions, which have a smaller number of participating nucleons. However, the results at forward rapidity show a similar suppression within uncertainties. The results in the integrated centrality are compared with calculations using nuclear parton distribution functions, which show a reasonable agreement at the forward rapidity but fail to describe the backward rapidity enhancement.
DOI: 10.17182/hepdata.106855.v1/t1
title: "Figure 8" of "Test of lepton universality in beauty-quark decays"

description: Likelihood function from the fit to the nonresonant $B^+$ --&gt; $K^+\ell^+ \ell^−$ candidates profiled as a function of $R_K$.
description: The Standard Model of particle physics currently provides our best description of fundamental particles and their interactions. The theory predicts that the different charged leptons, the electron, muon and tau, have identical electroweak interaction strengths. Previous measurements have shown a wide range of particle decays are consistent with this principle of lepton universality. This article presents evidence for the breaking of lepton universality in beauty-quark decays, with a significance of 3.1 standard deviations, based on proton-proton collision data collected with the LHCb detector at CERN’s Large Hadron Collider. The measurements are of processes in which a beauty meson transforms into a strange meson with the emission of either an electron and a positron, or a muon and an antimuon. If confirmed by future measurements, this violation of lepton universality would imply physics beyond the Standard Model, such as a new fundamental interaction between quarks and leptons.
DOI: 10.17182/hepdata.107754.v1/t1
title: "Table 1" of "Measurements of the electroweak diboson production cross sections in proton-proton collisions at $\sqrt{s} =$ 5.02 TeV using leptonic decays"

description: Expected event yields in the WW SR and observed number of events. The uncertainties correspond to the statistical and systematic component, respectively.
description: The first measurements of diboson production cross sections at a center-of-mass energy of $5.02~\mathrm{TeV}$ are reported. They are based on proton-proton collision data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $302~\mathrm{pb}^{-1}$. Events with two, three, or four charged light leptons (electrons or muons) in the final state are analyzed. The $\mathrm{WW}$, $\mathrm{WZ}$, and $\mathrm{ZZ}$ total cross sections are measured as $\sigma_{\mathrm{WW}}=37.0 \text{ }^{+5.5}_{-5.2} (\text{stat}) \text{ }^{+2.7}_{-2.6} (\text{syst})~\mathrm{pb}$, $\sigma_{\mathrm{WZ}}=6.4 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.3} (\text{syst})~\mathrm{pb}$, and $\sigma_{\mathrm{ZZ}}=5.3 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.4} (\text{syst})~\mathrm{pb}$. All measurements are in good agreement with theoretical calculations at combined next-to-next-to-leading order quantum chromodynamics and next-to-leading order electroweak accuracy.
DOI: 10.17182/hepdata.107754.v1/t2
title: "Table 2" of "Measurements of the electroweak diboson production cross sections in proton-proton collisions at $\sqrt{s} =$ 5.02 TeV using leptonic decays"

description: Expected event yields for the signal and total background in the WZ and ZZ SRs, and observed number of events. The uncertainties correspond to the statistical and systematic component, respectively.
description: The first measurements of diboson production cross sections at a center-of-mass energy of $5.02~\mathrm{TeV}$ are reported. They are based on proton-proton collision data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $302~\mathrm{pb}^{-1}$. Events with two, three, or four charged light leptons (electrons or muons) in the final state are analyzed. The $\mathrm{WW}$, $\mathrm{WZ}$, and $\mathrm{ZZ}$ total cross sections are measured as $\sigma_{\mathrm{WW}}=37.0 \text{ }^{+5.5}_{-5.2} (\text{stat}) \text{ }^{+2.7}_{-2.6} (\text{syst})~\mathrm{pb}$, $\sigma_{\mathrm{WZ}}=6.4 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.3} (\text{syst})~\mathrm{pb}$, and $\sigma_{\mathrm{ZZ}}=5.3 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.4} (\text{syst})~\mathrm{pb}$. All measurements are in good agreement with theoretical calculations at combined next-to-next-to-leading order quantum chromodynamics and next-to-leading order electroweak accuracy.
DOI: 10.17182/hepdata.107754.v1/t3
title: "Figure 1 Left" of "Measurements of the electroweak diboson production cross sections in proton-proton collisions at $\sqrt{s} =$ 5.02 TeV using leptonic decays"

description: Distribution of the dilepton pT in the WW signal region. Events from DY, conversions, and diboson processes are grouped into the 'Others' category. The vertical error bars represent the statistical uncertainty in the data and the shaded band the uncertainty in the prediction. The signal contributions are scaled to the measured cross sections (postfit).
description: The first measurements of diboson production cross sections at a center-of-mass energy of $5.02~\mathrm{TeV}$ are reported. They are based on proton-proton collision data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $302~\mathrm{pb}^{-1}$. Events with two, three, or four charged light leptons (electrons or muons) in the final state are analyzed. The $\mathrm{WW}$, $\mathrm{WZ}$, and $\mathrm{ZZ}$ total cross sections are measured as $\sigma_{\mathrm{WW}}=37.0 \text{ }^{+5.5}_{-5.2} (\text{stat}) \text{ }^{+2.7}_{-2.6} (\text{syst})~\mathrm{pb}$, $\sigma_{\mathrm{WZ}}=6.4 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.3} (\text{syst})~\mathrm{pb}$, and $\sigma_{\mathrm{ZZ}}=5.3 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.4} (\text{syst})~\mathrm{pb}$. All measurements are in good agreement with theoretical calculations at combined next-to-next-to-leading order quantum chromodynamics and next-to-leading order electroweak accuracy.
DOI: 10.17182/hepdata.107754.v1/t4
title: "Figure 1 Right" of "Measurements of the electroweak diboson production cross sections in proton-proton collisions at $\sqrt{s} =$ 5.02 TeV using leptonic decays"

description: Distribution of the W boson transverse mass in the WZ 3l signal region. Events from conversions, and DY processes are grouped into the 'Others' category. The vertical error bars represent the statistical uncertainty in the data and the shaded band the uncertainty in the prediction. The signal contributions are scaled to the measured cross sections (postfit).
description: The first measurements of diboson production cross sections at a center-of-mass energy of $5.02~\mathrm{TeV}$ are reported. They are based on proton-proton collision data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $302~\mathrm{pb}^{-1}$. Events with two, three, or four charged light leptons (electrons or muons) in the final state are analyzed. The $\mathrm{WW}$, $\mathrm{WZ}$, and $\mathrm{ZZ}$ total cross sections are measured as $\sigma_{\mathrm{WW}}=37.0 \text{ }^{+5.5}_{-5.2} (\text{stat}) \text{ }^{+2.7}_{-2.6} (\text{syst})~\mathrm{pb}$, $\sigma_{\mathrm{WZ}}=6.4 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.3} (\text{syst})~\mathrm{pb}$, and $\sigma_{\mathrm{ZZ}}=5.3 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.4} (\text{syst})~\mathrm{pb}$. All measurements are in good agreement with theoretical calculations at combined next-to-next-to-leading order quantum chromodynamics and next-to-leading order electroweak accuracy.
DOI: 10.17182/hepdata.107754.v1/t5
title: "Figure 2" of "Measurements of the electroweak diboson production cross sections in proton-proton collisions at $\sqrt{s} =$ 5.02 TeV using leptonic decays"

description: Results obtained in this analysis and other diboson production cross section measurements at different center-of-mass energies for the CMS, ATLAS, CDF, and D0 Collaborations are presented, and compared with the NNLO QCD x NLO EW and NLO predictions from MATRIX. The vertical error bars represent the uncertainty in the measured cross section.
description: The first measurements of diboson production cross sections at a center-of-mass energy of $5.02~\mathrm{TeV}$ are reported. They are based on proton-proton collision data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $302~\mathrm{pb}^{-1}$. Events with two, three, or four charged light leptons (electrons or muons) in the final state are analyzed. The $\mathrm{WW}$, $\mathrm{WZ}$, and $\mathrm{ZZ}$ total cross sections are measured as $\sigma_{\mathrm{WW}}=37.0 \text{ }^{+5.5}_{-5.2} (\text{stat}) \text{ }^{+2.7}_{-2.6} (\text{syst})~\mathrm{pb}$, $\sigma_{\mathrm{WZ}}=6.4 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.3} (\text{syst})~\mathrm{pb}$, and $\sigma_{\mathrm{ZZ}}=5.3 \text{ }^{+2.5}_{-2.1} (\text{stat}) \text{ }^{+0.5}_{-0.4} (\text{syst})~\mathrm{pb}$. All measurements are in good agreement with theoretical calculations at combined next-to-next-to-leading order quantum chromodynamics and next-to-leading order electroweak accuracy.
DOI: 10.17182/hepdata.107760.v1/t1
title: "Figure 3" of "Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector"

description: Post-fit results for all $m_\text{jj}$ SR and CR bins in the EW $Z \gamma + \text{jets}$ cross-section measurement with the $\mu_{Z \gamma_\text{EW}}$ signal normalization floating. The post-fit uncertainties include statistical, experimental, and theory contributions.
description: This paper presents a measurement of the electroweak production of two jets in association with a $Z\gamma$ pair, with the $Z$ boson decaying into two neutrinos. It also presents a search for invisible or partially invisible decays of a Higgs boson with a mass of 125 GeV produced through vector-boson fusion with a photon in the final state. These results use data from LHC proton-proton collisions at $\sqrt{s}$ = 13 TeV collected with the ATLAS detector and corresponding to an integrated luminosity of 139 fb$^{-1}$. The event signature, shared by all benchmark processes considered for the measurements and searches, is characterized by a significant amount of unbalanced transverse momentum and a photon in the final state, in addition to a pair of forward jets. Electroweak $Z\gamma$ production in association with two jets is obseved in this final state with a significance of 5.2 (5.1 expected) standard deviations. The measured fiducial cross-section for this process is 1.31 $\pm$ 0.29 fb. An observed (expected) upper limit of 0.37 (0.34) at 95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to invisible particles, assuming the Standard Model production cross-section. The signature is also interpreted in the context of decays of a Higgs boson into a photon and a dark photon. An observed (expected) 95% CL upper limit on the branching ratio for this decay is set at 0.018 (0.017), assuming the Standard Model production cross-section for a 125 GeV Higgs boson.
DOI: 10.17182/hepdata.107760.v1/t2
title: "Figure 4" of "Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector"

description: Post-fit results for all DNN SR and CR bins in the search for $H \to \text{inv.}$ with the $\mathcal{B}_\text{inv}$ signal normalization set to zero. For the $Z_\text{Rev.Cen.}^\gamma$ CR, the third bin contains all events with DNN output score values of 0.6-1.0. The $H \to \text{inv.}$ signal is scaled to a $\mathcal{B}_\text{inv}$ of 37%. The post-fit uncertainties include statistical, experimental, and theoretical contributions.
description: This paper presents a measurement of the electroweak production of two jets in association with a $Z\gamma$ pair, with the $Z$ boson decaying into two neutrinos. It also presents a search for invisible or partially invisible decays of a Higgs boson with a mass of 125 GeV produced through vector-boson fusion with a photon in the final state. These results use data from LHC proton-proton collisions at $\sqrt{s}$ = 13 TeV collected with the ATLAS detector and corresponding to an integrated luminosity of 139 fb$^{-1}$. The event signature, shared by all benchmark processes considered for the measurements and searches, is characterized by a significant amount of unbalanced transverse momentum and a photon in the final state, in addition to a pair of forward jets. Electroweak $Z\gamma$ production in association with two jets is obseved in this final state with a significance of 5.2 (5.1 expected) standard deviations. The measured fiducial cross-section for this process is 1.31 $\pm$ 0.29 fb. An observed (expected) upper limit of 0.37 (0.34) at 95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to invisible particles, assuming the Standard Model production cross-section. The signature is also interpreted in the context of decays of a Higgs boson into a photon and a dark photon. An observed (expected) 95% CL upper limit on the branching ratio for this decay is set at 0.018 (0.017), assuming the Standard Model production cross-section for a 125 GeV Higgs boson.
DOI: 10.17182/hepdata.107760.v1/t3
title: "Figure 5" of "Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector"

description: Post-fit results for the ten [$m_\text{jj}$, $m_\text{T}$] bins constituting the SR and CRs defined for the dark photon search with the $\mathcal{B}(H \to \gamma \gamma_\text{d})$ signal normalization set to zero. A $H \to \gamma \gamma_\text{d}$ signal is shown for two different mass hypotheses (125 GeV, 500 GeV) and scaled to a branching ratio of 2% and 1%, respectively. The post-fit uncertainties include statistical, experimental, and theoretical contributions.
description: This paper presents a measurement of the electroweak production of two jets in association with a $Z\gamma$ pair, with the $Z$ boson decaying into two neutrinos. It also presents a search for invisible or partially invisible decays of a Higgs boson with a mass of 125 GeV produced through vector-boson fusion with a photon in the final state. These results use data from LHC proton-proton collisions at $\sqrt{s}$ = 13 TeV collected with the ATLAS detector and corresponding to an integrated luminosity of 139 fb$^{-1}$. The event signature, shared by all benchmark processes considered for the measurements and searches, is characterized by a significant amount of unbalanced transverse momentum and a photon in the final state, in addition to a pair of forward jets. Electroweak $Z\gamma$ production in association with two jets is obseved in this final state with a significance of 5.2 (5.1 expected) standard deviations. The measured fiducial cross-section for this process is 1.31 $\pm$ 0.29 fb. An observed (expected) upper limit of 0.37 (0.34) at 95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to invisible particles, assuming the Standard Model production cross-section. The signature is also interpreted in the context of decays of a Higgs boson into a photon and a dark photon. An observed (expected) 95% CL upper limit on the branching ratio for this decay is set at 0.018 (0.017), assuming the Standard Model production cross-section for a 125 GeV Higgs boson.
DOI: 10.17182/hepdata.107760.v1/t4
title: "Figure 6" of "Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector"

description: Post-fit $m_\text{T}(\gamma, E_\text{T}^\text{miss})$ distribution in the inclusive signal region for the dark-photon search with the 125 GeV mass $\mathcal{B}(H \to \gamma \gamma_\text{d})$ signal normalization set to zero. A $H \to \gamma \gamma_\text{d}$ decay signal is shown for two different mass hypotheses, 125 GeV and 500 GeV, and scaled to a $\mathcal{B}(H \to \gamma \gamma_\text{d})$ of 2% and 1%, respectively. Events with $m_\text{T}(\gamma, E_\text{T}^\text{miss})$ larger than the rightmost bin boundary are added to that bin.
description: This paper presents a measurement of the electroweak production of two jets in association with a $Z\gamma$ pair, with the $Z$ boson decaying into two neutrinos. It also presents a search for invisible or partially invisible decays of a Higgs boson with a mass of 125 GeV produced through vector-boson fusion with a photon in the final state. These results use data from LHC proton-proton collisions at $\sqrt{s}$ = 13 TeV collected with the ATLAS detector and corresponding to an integrated luminosity of 139 fb$^{-1}$. The event signature, shared by all benchmark processes considered for the measurements and searches, is characterized by a significant amount of unbalanced transverse momentum and a photon in the final state, in addition to a pair of forward jets. Electroweak $Z\gamma$ production in association with two jets is obseved in this final state with a significance of 5.2 (5.1 expected) standard deviations. The measured fiducial cross-section for this process is 1.31 $\pm$ 0.29 fb. An observed (expected) upper limit of 0.37 (0.34) at 95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to invisible particles, assuming the Standard Model production cross-section. The signature is also interpreted in the context of decays of a Higgs boson into a photon and a dark photon. An observed (expected) 95% CL upper limit on the branching ratio for this decay is set at 0.018 (0.017), assuming the Standard Model production cross-section for a 125 GeV Higgs boson.
DOI: 10.17182/hepdata.107760.v1/t5
title: "Figure 7" of "Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector"

description: The 95% CL upper limit on the Higgs boson production cross-section times branching ratio to $\gamma \gamma_\text{d}$ is shown for different VBF-produced scalar-mediator-mass hypotheses in the NWA. The theoretically predicted cross-section of a Higgs boson produced via VBF and with the $\mathcal{B}(H \to \gamma \gamma_\text{d}) =$ 5% is superimposed on the $\pm 1\sigma$ and $\pm 2\sigma$ NNLO QCD + NLO EW uncertainty band of the expected production cross-section limit.
description: This paper presents a measurement of the electroweak production of two jets in association with a $Z\gamma$ pair, with the $Z$ boson decaying into two neutrinos. It also presents a search for invisible or partially invisible decays of a Higgs boson with a mass of 125 GeV produced through vector-boson fusion with a photon in the final state. These results use data from LHC proton-proton collisions at $\sqrt{s}$ = 13 TeV collected with the ATLAS detector and corresponding to an integrated luminosity of 139 fb$^{-1}$. The event signature, shared by all benchmark processes considered for the measurements and searches, is characterized by a significant amount of unbalanced transverse momentum and a photon in the final state, in addition to a pair of forward jets. Electroweak $Z\gamma$ production in association with two jets is obseved in this final state with a significance of 5.2 (5.1 expected) standard deviations. The measured fiducial cross-section for this process is 1.31 $\pm$ 0.29 fb. An observed (expected) upper limit of 0.37 (0.34) at 95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to invisible particles, assuming the Standard Model production cross-section. The signature is also interpreted in the context of decays of a Higgs boson into a photon and a dark photon. An observed (expected) 95% CL upper limit on the branching ratio for this decay is set at 0.018 (0.017), assuming the Standard Model production cross-section for a 125 GeV Higgs boson.