cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.144361.v2/t5
title: "Figure 2b" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the invariant mass of the transverse mass of the WW system after the signal region selection before the fit to data.The shaded band represents the Monte Carlo statistical unc
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (5.1) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 5.9 \pm 0.8 \text{(stat)} \pm 0.8 \text{(syst)} \pm 0.7 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v2/t6
title: "Figure 3a" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The unrolled two-dimensional mTWW-mll$\gamma$ distributions with category 0 jet after the fit to data. The data are compared to the sum of the signal and expected background. The black points with error bars represent the data and their statistical uncertainties, whereas the hatched bands represent the total uncertainties in the predictions.
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (5.1) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 5.9 \pm 0.8 \text{(stat)} \pm 0.8 \text{(syst)} \pm 0.7 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v2/t7
title: "Figure 3b" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The unrolled two-dimensional mTWW-mll$\gamma$ distributions with category 1more jets after the fit to data. The data are compared to the sum of the signal and expected background. The black points with error bars represent the data and their statistical uncertainties, whereas the hatched bands represent the total uncertainties in the predictions.
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (5.1) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 5.9 \pm 0.8 \text{(stat)} \pm 0.8 \text{(syst)} \pm 0.7 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v1/t1
title: "Table 1" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The number of events in data and simulations after the fit to data in the Top$\gamma$ CR, SS$WW\gamma$ CR, and signal region.
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (4.7) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 6.0 \pm 0.8 \text{(stat)} \pm 0.7 \text{(syst)} \pm 0.6 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v1/t2
title: "Table 2" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Upper limits on the cross section and derived limits in terms of Yukawa coupling at 95% CL for Hγ production initiated by light quarks.
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (4.7) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 6.0 \pm 0.8 \text{(stat)} \pm 0.7 \text{(syst)} \pm 0.6 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v1/t3
title: "Figure 2a" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the invariant mass of the dilepton-photon system after the signal region selection before the fit to data.The shaded band represents the Monte Carlo statistical unc
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (4.7) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 6.0 \pm 0.8 \text{(stat)} \pm 0.7 \text{(syst)} \pm 0.6 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v1/t4
title: "Figure 2b" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the invariant mass of the transverse mass of the WW system after the signal region selection before the fit to data.The shaded band represents the Monte Carlo statistical unc
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (4.7) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 6.0 \pm 0.8 \text{(stat)} \pm 0.7 \text{(syst)} \pm 0.6 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v1/t5
title: "Figure 3a" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The unrolled two-dimensional mTWW-mll$\gamma$ distributions with category 0 jet after the fit to data. The data are compared to the sum of the signal and expected background. The black points with error bars represent the data and their statistical uncertainties, whereas the hatched bands represent the total uncertainties in the predictions.
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (4.7) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 6.0 \pm 0.8 \text{(stat)} \pm 0.7 \text{(syst)} \pm 0.6 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.17182/hepdata.144361.v1/t6
title: "Figure 3b" of "Observation of WW$\gamma$ production and search for H$\gamma$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The unrolled two-dimensional mTWW-mll$\gamma$ distributions with category 1more jets after the fit to data. The data are compared to the sum of the signal and expected background. The black points with error bars represent the data and their statistical uncertainties, whereas the hatched bands represent the total uncertainties in the predictions.
description: The observation of $WW\gamma$ production in proton-proton collisions at a center-of-mass energy of 13\TeV with an integrated luminosity of 138\fbinv is presented. The observed (expected) significance is 5.6 (4.7) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for $WW\gamma$ is $ 6.0 \pm 0.8 \text{(stat)} \pm 0.7 \text{(syst)} \pm 0.6 \text{(modeling)} fb$, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
DOI: 10.5281/zenodo.17527057
title: Cyanophage Abundances and Infection Levels of Prochlorococcus and Synechococcus KM1502

description: Cyanophage Abundances and Infection Levels of Prochlorococcus and Synechococcus

This dataset collection of cyanophage abundances and infection levels of Prochlorococcus and Synechococcus was collected from the KM1502 (2015 SCOPE Transect) cruise in the Pacific Ocean. Cyanophage abundances and infection levels were analyzed using the polony and ipolony methods, respectively. These methods are a single-virus or single-cell assay that employs degenerate primers and probes to detect viruses or virus-infected cells belonging to a distinct cyanophage family.  The timestamp is in UTC.
DOI: 10.5281/zenodo.17527301
title: Cyanophage Abundances and Infection Levels of Prochlorococcus and Synechococcus KM1502

description: Cyanophage Abundances and Infection Levels of Prochlorococcus and Synechococcus

This dataset collection of cyanophage abundances and infection levels of Prochlorococcus and Synechococcus was collected from the KM1502 (2015 SCOPE Transect) cruise in the Pacific Ocean. Cyanophage abundances and infection levels were analyzed using the polony and ipolony methods, respectively. These methods are a single-virus or single-cell assay that employs degenerate primers and probes to detect viruses or virus-infected cells belonging to a distinct cyanophage family.  The timestamp is in UTC.
DOI: 10.17182/hepdata.144439.v1/t2
title: "mass_obs" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed exclusion limits at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t3
title: "mass_obs_plus" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed exclusion limits at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$ and a $+1 \sigma$ deviation of the NNLO+NNLL theoretical cross-section of a $\tilde{t}_1$ pair-production.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t4
title: "mass_obs_minus" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed exclusion limits at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$ and a $-1 \sigma$ deviation of the NNLO+NNLL theoretical cross-section of a $\tilde{t}_1$ pair-production.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t5
title: "mass_exp" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Expected exclusion limits at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t6
title: "mass_band_1" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: The $1\sigma$ variation of expected 95% CL exclusion contour obtained by varying MC statistical uncertainties, detector-related systematic uncertainties, and theoretical uncertainties in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t7
title: "mass_band_2" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: The $2\sigma$ variation of expected 95%CL exclusion contour obtained by varying MC statistical uncertainties, detector-related systematic uncertainties, and theoretical uncertainties in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t8
title: "br_m1_obs" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed exclusion limits at the 95% CL in the $m_{\tilde{t}_1} - $BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1)$ plane, assuming $m_{\tilde\chi^0_1} = 1 \mathrm{GeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t9
title: "br_m1_obs_plus" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed exclusion limits at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming $m_{\tilde\chi^0_1} = 1 \mathrm{ GeV}$ and a $+1 \sigma$ deviation of the NNLO+NNLL theoretical cross-section of a $\tilde{t}_1$ pair-production.
description: No data abstract available.
DOI: 10.5281/zenodo.17527284
title: L'impact de la concentration de l'actionnariat institutionnel sur l'inclusion des entreprises cotées dans l'indice MASI ESG

description: Cet article analyse l’effet de la concentration de l’actionnariat institutionnel sur l’inclusion des entreprises cotées dans l’indice MASI ESG de la Bourse de Casablanca. L’étude porte sur un échantillon de 60 entreprises marocaines observées sur la période 2019–2024. La méthodologie adoptée repose sur un modèle de régression logistique binaire (logit), dans lequel la variable dépendante mesure l’appartenance ou non d’une entreprise à l’indice ESG. La variable explicative principale est le pourcentage d’actionnariat institutionnel, tandis que la taille de l’entreprise, sa rentabilité (ROA) et son niveau d’endettement sont intégrés comme variables de contrôle. Les données ont été collectées à partir des rapports financiers disponibles auprès de l’Autorité Marocaine du Marché des Capitaux (AMMC). Les résultats empiriques mettent en évidence une relation positive et significative entre la concentration de l’actionnariat institutionnel et l’inclusion dans le MASI ESG, et montrent que la taille et l’endettement exercent également un effet positif sur cette inclusion, contrairement à la rentabilité qui reste non significative.
DOI: 10.5281/zenodo.17527285
title: L'impact de la concentration de l'actionnariat institutionnel sur l'inclusion des entreprises cotées dans l'indice MASI ESG

description: Cet article analyse l’effet de la concentration de l’actionnariat institutionnel sur l’inclusion des entreprises cotées dans l’indice MASI ESG de la Bourse de Casablanca. L’étude porte sur un échantillon de 60 entreprises marocaines observées sur la période 2019–2024. La méthodologie adoptée repose sur un modèle de régression logistique binaire (logit), dans lequel la variable dépendante mesure l’appartenance ou non d’une entreprise à l’indice ESG. La variable explicative principale est le pourcentage d’actionnariat institutionnel, tandis que la taille de l’entreprise, sa rentabilité (ROA) et son niveau d’endettement sont intégrés comme variables de contrôle. Les données ont été collectées à partir des rapports financiers disponibles auprès de l’Autorité Marocaine du Marché des Capitaux (AMMC). Les résultats empiriques mettent en évidence une relation positive et significative entre la concentration de l’actionnariat institutionnel et l’inclusion dans le MASI ESG, et montrent que la taille et l’endettement exercent également un effet positif sur cette inclusion, contrairement à la rentabilité qui reste non significative.
DOI: 10.17182/hepdata.144439.v1/t10
title: "br_m1_obs_minus" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed exclusion limits at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming $m_{\tilde\chi^0_1} = 1 \mathrm{ GeV}$ and a $-1 \sigma$ deviation of the NNLO+NNLL theoretical cross-section of a $\tilde{t}_1$ pair-production.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t11
title: "br_m1_exp" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Expected exclusion limits at the 95% CL in the $m_{\tilde{t}_1} - $BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1)$ plane, assuming $m_{\tilde\chi^0_1} = 1 \mathrm{GeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t12
title: "br_m1_band_1" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: The $1\sigma$ variation of expected 95% CL exclusion contour obtained by varying MC statistical uncertainties, detector-related systematic uncertainties, and theoretical uncertainties in the $m_{\tilde{t}_1} - $BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1)$ plane, assuming $m_{\tilde\chi^0_1} = 1 \mathrm{GeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t13
title: "br_m1_band_2" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: The $2\sigma$ variation of expected 95%CL exclusion contour obtained by varying MC statistical uncertainties, detector-related systematic uncertainties, and theoretical uncertainties in the $m_{\tilde{t}_1} - $BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1)$ plane, assuming $m_{\tilde\chi^0_1} = 1 \mathrm{GeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t14
title: "mass_upperLimits_obs" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed upper limits on the top-spartner pair production cross-section in fb at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t15
title: "mass_upperLimits_exp" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Expected upper limits on the top-spartner pair production cross-section in fb at the 95% CL in the $\tilde{t}_1 - \tilde\chi^0_1$ mass plane, assuming BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1) = 0.5$
description: No data abstract available.
DOI: 10.17182/hepdata.144439.v1/t16
title: "br_m1_upperLimits_obs" of "A search for top-squark pair production, in final states containing a top quark, a charm quark and missing transverse momentum, using the 139 fb$^{-1}$ of $pp$ collision data collected by the ATLAS detector"

description: Observed upper limits on the top-spartner pair production cross-section in fb at the 95% CL in the $m_{\tilde{t}_1} - $BR$(\tilde{t}_1 \rightarrow t + \tilde\chi^0_1)$ plane, assuming $m_{\tilde\chi^0_1} = 1 \mathrm{GeV}$.
description: No data abstract available.