cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.157553.v1/t62
title: "Cutflow for SROS-on" of "Search for cascade decays of charged sleptons and sneutrinos in final states with three leptons and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Summary of the number of events passing each selection for the $m(\tilde{\ell}_{\text{L}}^{\pm},\tilde{\chi}^0_3,\tilde{\chi}^0_1)=(300, 200, 100)$, $(550, 300, 100)$, $(450, 180, 100)$ GeV signal points, including all production processes. After the initial selections, the table is split into row blocks per inclusive region, and then further for each SR channel. Flavor-binned SRs are shown for SROS-on-b for reference. The generator level selections require to have two or more leptons.
description: No data abstract available.
DOI: 10.17182/hepdata.157553.v1/t63
title: "Cutflow for SROS-off" of "Search for cascade decays of charged sleptons and sneutrinos in final states with three leptons and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Summary of the number of events passing each selection for the $m(\tilde{\ell}_{\text{L}}^{\pm},\tilde{\chi}^0_3,\tilde{\chi}^0_1)=(300, 200, 100)$, $(550, 300, 100)$, $(450, 180, 100)$ GeV signal points, including all production processes. After the initial selections, the table is split into row blocks per inclusive region, and then further for each SR channel. Flavor-binned SRs are shown for SROS-off-b for reference. The generator level selections require to have two or more leptons.
description: No data abstract available.
DOI: 10.17182/hepdata.157553.v1/t64
title: "Cutflow for SRSS" of "Search for cascade decays of charged sleptons and sneutrinos in final states with three leptons and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Summary of the number of events passing each selection for the $m(\tilde{\ell}_{\text{L}}^{\pm},\tilde{\chi}^0_3,\tilde{\chi}^0_1)=(300, 200, 100)$, $(550, 300, 100)$, $(450, 180, 100)$ GeV signal points, including all production processes. After the initial selections, the table is split into row blocks per inclusive region, and then further for each SR channel. Flavor-binned SRs are shown. The generator level selections require to have two or more leptons.
description: No data abstract available.
DOI: 10.17182/hepdata.157577.v1/t2
title: "Figure 7 correlation matrix" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Example description
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157577.v1/t1
title: "Figure 7" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Differential fiducial cross sections for pT of the Higgs boson
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157577.v1/t3
title: "Figure 8" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Differential fiducial cross sections for rapidity of the Higgs boson
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157577.v1/t4
title: "Figure 8 correlation matrix" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Example description
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157577.v1/t5
title: "Figure 9" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Differential fiducial cross sections for the number of jets
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157577.v1/t6
title: "Figure 9 correlation matrix" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Example description
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157577.v1/t7
title: "Figure 10" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Differential fiducial cross sections for the leading jet pT
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157577.v1/t8
title: "Figure 10 correlation matrix" of "Measurements of inclusive and differential Higgs boson production cross sections at $\sqrt{s}$ = 13.6 TeV in the H $\to$$γγ$ decay channel"

description: Example description
description: Inclusive and differential cross sections for the Higgs boson production in proton-proton collisions at a centre-of-mass energy of 13.6 TeV are measured. The data set was collected with the CMS detector at the LHC in 2022 and corresponds to an integrated luminosity of $34.7~\mathrm{fb}^{-1}$. Events with the diphoton final state are selected, and the measured inclusive fiducial cross section is $\sigma_{fid} = 74 \pm 11~\text{(stat)}^{+5}_{−4}~\text{(syst)}~\mathrm{fb}$, in agreement with the standard model prediction of $67.8 \pm 3.8~\mathrm{fb}$$. Differential cross sections are measured as functions of several observables: the Higgs boson transverse momentum and rapidity, the number of associated jets, and the transverse momentum of the leading jet in the event. The differential cross sections also agree with the standard model predictions within the uncertainties.
DOI: 10.17182/hepdata.157586.v1/t1
title: "Figure 10a" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Unfolded Lund Jet Plane in the top jet selection.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t2
title: "Figures 11a & 13a" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Unfolded Lund Jet Plane in the top jet selection, $2.11&lt;\ln(1/z)&lt;2.46$.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t3
title: "Figures 11b & 13b" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Unfolded Lund Jet Plane in the top jet selection, $1.60&lt;\ln(R/\Delta R)&lt;2.00$.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t4
title: "Total covariance (top jets)" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Total covariance matrix for the unfolded Lund Jet Plane in the top jet selection.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t5
title: "Stat. covariance (top jets)" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Statistical covariance matrix for the unfolded Lund Jet Plane in the top jet selection.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t6
title: "Figure 10b" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Unfolded Lund Jet Plane in the W jet selection.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t10
title: "Stat. covariance (W jets)" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Statistical covariance matrix for the unfolded Lund Jet Plane in the W jet selection.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t7
title: "Figures 12a & 14a" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Unfolded Lund Jet Plane in the W jet selection, $2.11&lt;\ln(1/z)&lt;2.46$.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t8
title: "Figures 12b & 14b" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Unfolded Lund Jet Plane in the W jet selection, $1.60&lt;\ln(R/\Delta R)&lt;2.00$.
description: No data abstract available.
DOI: 10.17182/hepdata.157586.v1/t9
title: "Total covariance (W jets)" of "Measurement of the Lund jet plane in hadronic decays of top quarks and W bosons with the ATLAS detector"

description: Total covariance matrix for the unfolded Lund Jet Plane in the W jet selection.
description: No data abstract available.
DOI: 10.17182/hepdata.157601.v1/t1
title: "Figure 2a" of "Observation of WZ$\gamma$ production and constraints on new physics scenarios in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the variables used in the simultaneous fit for the nonprompt $l$ CR. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the predicted uncertainties. The bottom panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction. The last bin of each plot has been extended to include the overflow contribution.
description: No data abstract available.
DOI: 10.17182/hepdata.157601.v1/t2
title: "Figure 2b" of "Observation of WZ$\gamma$ production and constraints on new physics scenarios in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the variables used in the simultaneous fit for the nonprompt $\gamma$ CR. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the predicted uncertainties. The bottom panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction. The last bin of each plot has been extended to include the overflow contribution.
description: No data abstract available.
DOI: 10.17182/hepdata.157601.v1/t3
title: "Figure 2c" of "Observation of WZ$\gamma$ production and constraints on new physics scenarios in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the variables used in the simultaneous fit for the ZZ CR. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the predicted uncertainties. The bottom panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction. The last bin of each plot has been extended to include the overflow contribution.
description: No data abstract available.
DOI: 10.17182/hepdata.157601.v1/t4
title: "Figure 2d" of "Observation of WZ$\gamma$ production and constraints on new physics scenarios in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the variables used in the simultaneous fit for the SR. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the predicted uncertainties. The bottom panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction. The last bin of each plot has been extended to include the overflow contribution.
description: No data abstract available.
DOI: 10.17182/hepdata.157601.v1/t5
title: "Figure 3A" of "Observation of WZ$\gamma$ production and constraints on new physics scenarios in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the cross section and branching fraction$\sigma(\mathrm{pp} \
ightarrow W\mathrm{a})\mathcal{B}(W 
ightarrow \ell^{+}
v_{\ell})\mathcal{B}(\mathrm{a} \rightarrow Z\gamma)\mathcal{B}(Z \rightarrow \ell^{+} \ell^{-})$ s a function of the ALP mass from 110 to 400 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.157601.v1/t6
title: "Figure 3B" of "Observation of WZ$\gamma$ production and constraints on new physics scenarios in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the photophobic ALP model parameter $1/f_{\mathrm{a}}$ as a function of ALP mass reinterpreted from $1/f_{\mathrm{a}}=2~\mathrm{TeV}^{-1}$
description: No data abstract available.
DOI: 10.17182/hepdata.157781.v1/t1
title: "Diphoton invariant mass" of "Search for Higgs boson decays into a pair of pseudoscalar particles in the $\gamma\gamma\tau_{\text{had}}\tau_{\text{had}}$ final state using $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Distribution of the diphoton invariant mass for all events satisfying the analysis selections in the full Run 2 dataset.
description: No data abstract available.
DOI: 10.17182/hepdata.157781.v1/t2
title: "Local $p$-value" of "Search for Higgs boson decays into a pair of pseudoscalar particles in the $\gamma\gamma\tau_{\text{had}}\tau_{\text{had}}$ final state using $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Scan of the observed $p$-value as a function of $m_{a}$ for the background-only hypothesis.
description: No data abstract available.
DOI: 10.17182/hepdata.157781.v1/t3
title: "Upper limits on the branching ratio (expected $\pm1\sigma$)" of "Search for Higgs boson decays into a pair of pseudoscalar particles in the $\gamma\gamma\tau_{\text{had}}\tau_{\text{had}}$ final state using $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The observed and expected ($\pm1\sigma$) upper limits at 95% CL on the branching ratio for $H\rightarrow aa\rightarrow \gamma\gamma\tau\tau$ as a function of the resonance mass hypothesis $m_{a}$.
description: No data abstract available.
DOI: 10.17182/hepdata.157781.v1/t4
title: "Upper limits on the branching ratio (expected $\pm2\sigma$)" of "Search for Higgs boson decays into a pair of pseudoscalar particles in the $\gamma\gamma\tau_{\text{had}}\tau_{\text{had}}$ final state using $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The observed and expected ($\pm2\sigma$) upper limits at 95% CL on the branching ratio for $H\rightarrow aa\rightarrow \gamma\gamma\tau\tau$ as a function of the resonance mass hypothesis $m_{a}$.
description: No data abstract available.
DOI: 10.17182/hepdata.157781.v1/t5
title: "Signal selection efficiency" of "Search for Higgs boson decays into a pair of pseudoscalar particles in the $\gamma\gamma\tau_{\text{had}}\tau_{\text{had}}$ final state using $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The polynomial parameterisation of the total signal selection efficiency as a function of $m_{a}$, defined as the fraction of the reconstructed and selected events out of the total number of events in the signal simulated samples.
description: No data abstract available.
DOI: 10.17182/hepdata.157849.v1/t1
title: "Summary" of "Probing the flavour structure of dimension-6 EFT operators in multilepton final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Summary of the limits obtained for the Wilson coefficients.
description: An analysis of the flavour structure of dimension-6 effective field theory (EFT) operators in multilepton final states is presented, focusing on the interactions involving Z bosons. The flavour structure of these operators is disentangled by simultaneously probing the interactions with different quark generations in final states with at least three leptons, targetting the associated production of a top quark pair and a Z boson (ttZ) as well as diboson processes (WZ and ZZ). The data were recorded by the CMS experiment in the years 2016 to 2018 in proton-proton collisions at a centre-of-mass energy of 13 TeV and correspond to an integrated luminosity of $138\;\mathrm{fb}^{-1}$. Consistency with the standard model of particle physics is observed and limits on the considered EFT parameters, split into couplings to light and heavy quark generations, are set.
DOI: 10.17182/hepdata.157849.v1/t2
title: "Likelihood cHqMRe1122 cHqMRe33 fixed" of "Probing the flavour structure of dimension-6 EFT operators in multilepton final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Likelihood scan of cHqMRe1122 versus cHqMRe33. Other Wilson coefficients are fixed to zero.
description: An analysis of the flavour structure of dimension-6 effective field theory (EFT) operators in multilepton final states is presented, focusing on the interactions involving Z bosons. The flavour structure of these operators is disentangled by simultaneously probing the interactions with different quark generations in final states with at least three leptons, targetting the associated production of a top quark pair and a Z boson (ttZ) as well as diboson processes (WZ and ZZ). The data were recorded by the CMS experiment in the years 2016 to 2018 in proton-proton collisions at a centre-of-mass energy of 13 TeV and correspond to an integrated luminosity of $138\;\mathrm{fb}^{-1}$. Consistency with the standard model of particle physics is observed and limits on the considered EFT parameters, split into couplings to light and heavy quark generations, are set.