cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.127765.v1/t19
title: "Decay channel signal strength modifiers correlations" of "A portrait of the Higgs boson by the CMS experiment ten years after the discovery"

description: Observed correlations between the signal strength modifiers per decay channel, $\mu^f$
description: CERN-LHC. Higgs boson turns 10: results from the CMS experiment.
DOI: 10.17182/hepdata.127765.v1/t20
title: "Production times decay signal strength modifiers correlations" of "A portrait of the Higgs boson by the CMS experiment ten years after the discovery"

description: Observed correlations between the signal strength modifiers per production mode times decay channel $\mu_i^f$.
description: CERN-LHC. Higgs boson turns 10: results from the CMS experiment.
DOI: 10.17182/hepdata.127765.v1/t22
title: "Couplings effective loop correlations" of "A portrait of the Higgs boson by the CMS experiment ten years after the discovery"

description: Observed correlations between the coupling modifiers in the effective loop model
description: CERN-LHC. Higgs boson turns 10: results from the CMS experiment.
DOI: 10.17182/hepdata.127765.v1/t17
title: "KL-C2V (95)" of "A portrait of the Higgs boson by the CMS experiment ten years after the discovery"

description: Simultaneous coupling measurement $\kappa_\lambda/\kappa_{2V}$
description: CERN-LHC. Higgs boson turns 10: results from the CMS experiment.
DOI: 10.17182/hepdata.127766.v1/t1
title: "Figure 3a" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background prediction vs. observation in the b-veto signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t3
title: "Figure 3b" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background prediction vs. observation in the WH signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t4
title: "Figure 3b ratios" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background observation/prediction in the WH signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.25549/vercoutere-ouc113056751
title: Publisher correspondence

description: Correspondence between Al Vercoutere and various publishers related to publication of patient artwork in textbooks. Arranged in chronological order includes letters and forms (101), check receipts (9), and envelopes (15)
DOI: 10.17182/hepdata.127766.v1/t10
title: "Figure 4a Expected Lines" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: Expected exclusion limits assuming the approximate-NLO+NLL cross sections
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t2
title: "Figure 3a ratios" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background observation/prediction in the bVeto signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t5
title: "Figure 3c" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background prediction vs. observation in the W signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t6
title: "Figure 3c ratios" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background observation/prediction in the W signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t7
title: "Figure 3d" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background prediction vs. observation in the H signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t8
title: "Figure 3d ratios" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: SM background observation/prediction in the H signal region
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t9
title: "Figure 4a Observed Lines" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: Observed exclusion limits assuming the approximate-NLO+NLL cross sections
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127765.v1/t21
title: "Couplings resolved loop correlations" of "A portrait of the Higgs boson by the CMS experiment ten years after the discovery"

description: Observed correlations between the coupling modifiers in the resolved loop model
description: CERN-LHC. Higgs boson turns 10: results from the CMS experiment.
DOI: 10.17182/hepdata.127766.v1/t11
title: "Figure 4a Observed" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: The 95% CL observed upper limits on the production cross sections for $\widetilde{\chi}^\pm_1$ $\widetilde{\chi}^\mp_1$ assuming that each $\widetilde{\chi}^\pm_1$ decays to a W boson and $\widetilde{\chi}^0_1$
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.
DOI: 10.17182/hepdata.127766.v1/t12
title: "Figure 4b Observed Lines" of "Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum"

description: Observed exclusion limits assuming the approximate-NLO+NLL cross sections
description: Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.