cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.166317.v1/t5
title: "Table 5" of "Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The prompt production yield ratios between $\Xi_c^0$ and $\rm {D}^0$ measured in the same multiplicity classes.
description: The first measurement at midrapidity ($|y| &lt;~ 0.5$) of the production yield of the strange-charm baryons $\Xi_c^+$ and $\Xi_c^0$ as a function of transverse momentum ($p_{\rm T}$) in different charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ALICE experiment at the LHC is reported. The $\Xi_c^+$ baryon is reconstructed via the $\Xi_c^+ \rightarrow \Xi^-\pi^+\pi^+$ decay channel in the range $4 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$, while the $\Xi_c^0$ baryon is reconstructed via both the $\Xi_c^0 \rightarrow \Xi^-\pi^+$ and $\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$ decay channels in the range $2 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$. The baryon-to-meson ($\Xi_c^{0,+}/D^0$) and the baryon-to-baryon ($\Xi_c^{0,+}/\Lambda_c^+$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at $e^+e^-$ and $e^-$p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed. Moreover, the branching-fraction ratio of BR($\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$)/BR($\Xi_c^0 \rightarrow \Xi^-\pi^+$) is measured as 0.825 $\pm$ 0.094 (stat.) $\pm$ 0.081 (syst.). This value supersedes the previous ALICE measurement, improving the statistical precision by a factor of 1.6.
DOI: 10.17182/hepdata.166317.v1/t3
title: "Table 3" of "Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: Ratio between the prompt $\Xi_c^0$ baryons in a multiplicity class to the multiplicity-integrated (INEL $&gt;$ 0) class.
description: The first measurement at midrapidity ($|y| &lt;~ 0.5$) of the production yield of the strange-charm baryons $\Xi_c^+$ and $\Xi_c^0$ as a function of transverse momentum ($p_{\rm T}$) in different charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ALICE experiment at the LHC is reported. The $\Xi_c^+$ baryon is reconstructed via the $\Xi_c^+ \rightarrow \Xi^-\pi^+\pi^+$ decay channel in the range $4 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$, while the $\Xi_c^0$ baryon is reconstructed via both the $\Xi_c^0 \rightarrow \Xi^-\pi^+$ and $\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$ decay channels in the range $2 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$. The baryon-to-meson ($\Xi_c^{0,+}/D^0$) and the baryon-to-baryon ($\Xi_c^{0,+}/\Lambda_c^+$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at $e^+e^-$ and $e^-$p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed. Moreover, the branching-fraction ratio of BR($\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$)/BR($\Xi_c^0 \rightarrow \Xi^-\pi^+$) is measured as 0.825 $\pm$ 0.094 (stat.) $\pm$ 0.081 (syst.). This value supersedes the previous ALICE measurement, improving the statistical precision by a factor of 1.6.
DOI: 10.17182/hepdata.166317.v1/t6
title: "Table 6" of "Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The prompt production yield ratios between $\Xi_c^+$ and $\rm {D}^0$ measured in the same multiplicity classes.
description: The first measurement at midrapidity ($|y| &lt;~ 0.5$) of the production yield of the strange-charm baryons $\Xi_c^+$ and $\Xi_c^0$ as a function of transverse momentum ($p_{\rm T}$) in different charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ALICE experiment at the LHC is reported. The $\Xi_c^+$ baryon is reconstructed via the $\Xi_c^+ \rightarrow \Xi^-\pi^+\pi^+$ decay channel in the range $4 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$, while the $\Xi_c^0$ baryon is reconstructed via both the $\Xi_c^0 \rightarrow \Xi^-\pi^+$ and $\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$ decay channels in the range $2 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$. The baryon-to-meson ($\Xi_c^{0,+}/D^0$) and the baryon-to-baryon ($\Xi_c^{0,+}/\Lambda_c^+$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at $e^+e^-$ and $e^-$p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed. Moreover, the branching-fraction ratio of BR($\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$)/BR($\Xi_c^0 \rightarrow \Xi^-\pi^+$) is measured as 0.825 $\pm$ 0.094 (stat.) $\pm$ 0.081 (syst.). This value supersedes the previous ALICE measurement, improving the statistical precision by a factor of 1.6.
DOI: 10.17182/hepdata.166317.v1/t7
title: "Table 7" of "Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The prompt production yield ratios between $\Xi_c^0$ and $\Lambda_c^+$ measured in the same multiplicity classes.
description: The first measurement at midrapidity ($|y| &lt;~ 0.5$) of the production yield of the strange-charm baryons $\Xi_c^+$ and $\Xi_c^0$ as a function of transverse momentum ($p_{\rm T}$) in different charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ALICE experiment at the LHC is reported. The $\Xi_c^+$ baryon is reconstructed via the $\Xi_c^+ \rightarrow \Xi^-\pi^+\pi^+$ decay channel in the range $4 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$, while the $\Xi_c^0$ baryon is reconstructed via both the $\Xi_c^0 \rightarrow \Xi^-\pi^+$ and $\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$ decay channels in the range $2 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$. The baryon-to-meson ($\Xi_c^{0,+}/D^0$) and the baryon-to-baryon ($\Xi_c^{0,+}/\Lambda_c^+$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at $e^+e^-$ and $e^-$p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed. Moreover, the branching-fraction ratio of BR($\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$)/BR($\Xi_c^0 \rightarrow \Xi^-\pi^+$) is measured as 0.825 $\pm$ 0.094 (stat.) $\pm$ 0.081 (syst.). This value supersedes the previous ALICE measurement, improving the statistical precision by a factor of 1.6.
DOI: 10.17182/hepdata.166317.v1/t8
title: "Table 8" of "Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The prompt production yield ratios between $\Xi_c^+$ and $\Lambda_c^+$ measured in the same multiplicity classes.
description: The first measurement at midrapidity ($|y| &lt;~ 0.5$) of the production yield of the strange-charm baryons $\Xi_c^+$ and $\Xi_c^0$ as a function of transverse momentum ($p_{\rm T}$) in different charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ALICE experiment at the LHC is reported. The $\Xi_c^+$ baryon is reconstructed via the $\Xi_c^+ \rightarrow \Xi^-\pi^+\pi^+$ decay channel in the range $4 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$, while the $\Xi_c^0$ baryon is reconstructed via both the $\Xi_c^0 \rightarrow \Xi^-\pi^+$ and $\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$ decay channels in the range $2 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$. The baryon-to-meson ($\Xi_c^{0,+}/D^0$) and the baryon-to-baryon ($\Xi_c^{0,+}/\Lambda_c^+$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at $e^+e^-$ and $e^-$p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed. Moreover, the branching-fraction ratio of BR($\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$)/BR($\Xi_c^0 \rightarrow \Xi^-\pi^+$) is measured as 0.825 $\pm$ 0.094 (stat.) $\pm$ 0.081 (syst.). This value supersedes the previous ALICE measurement, improving the statistical precision by a factor of 1.6.
DOI: 10.17182/hepdata.166317.v1/t9
title: "Table 9" of "Multiplicity dependence of $Ξ_c^+$ and $Ξ_c^0$ production in pp collisions at $\sqrt{s} = 13$ TeV"

description: The branching-fraction ratio of BR($\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$)/BR($\Xi_c^0 \rightarrow \Xi^-\pi^+$)
description: The first measurement at midrapidity ($|y| &lt;~ 0.5$) of the production yield of the strange-charm baryons $\Xi_c^+$ and $\Xi_c^0$ as a function of transverse momentum ($p_{\rm T}$) in different charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ALICE experiment at the LHC is reported. The $\Xi_c^+$ baryon is reconstructed via the $\Xi_c^+ \rightarrow \Xi^-\pi^+\pi^+$ decay channel in the range $4 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$, while the $\Xi_c^0$ baryon is reconstructed via both the $\Xi_c^0 \rightarrow \Xi^-\pi^+$ and $\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$ decay channels in the range $2 &lt;~ p_{\rm T} &lt;~ 12$ GeV/$c$. The baryon-to-meson ($\Xi_c^{0,+}/D^0$) and the baryon-to-baryon ($\Xi_c^{0,+}/\Lambda_c^+$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at $e^+e^-$ and $e^-$p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed. Moreover, the branching-fraction ratio of BR($\Xi_c^0 \rightarrow \Xi^-e^+\nu_e$)/BR($\Xi_c^0 \rightarrow \Xi^-\pi^+$) is measured as 0.825 $\pm$ 0.094 (stat.) $\pm$ 0.081 (syst.). This value supersedes the previous ALICE measurement, improving the statistical precision by a factor of 1.6.
DOI: 10.17182/hepdata.103058.v1/t1
title: "Table 1" of "Longitudinal Double-Spin Asymmetries for $\pi^{0}$s in the Forward Direction for 510 GeV Polarized $pp$ Collisions"

description: Longitudinal Double-Spin Asymmetry, $A_{LL}$ vs $\pi^0$ transverse momentum in polarized pp collisions at $\sqrt{s}$ = 510 GeV. $\pm 6.7\%$ polarization scale uncertainty not shown.
description: The STAR Collaboration reports measurements of the longitudinal double-spin asymmetry, $A_{LL}$, for neutral pions produced at forward directions in polarized proton-proton collisions, at a center-of-mass energy of 510 GeV. Results are given for transverse momenta in the range $2
DOI: 10.17182/hepdata.103058.v1/t2
title: "Table 2" of "Longitudinal Double-Spin Asymmetries for $\pi^{0}$s in the Forward Direction for 510 GeV Polarized $pp$ Collisions"

description: Longitudinal Double-Spin Asymmetry, $A_{LL}$ vs $\pi^0$ transverse momentum in polarized pp collisions at $\sqrt{s}$ = 510 GeV. $\pm 6.7\%$ polarization scale uncertainty not shown.
description: The STAR Collaboration reports measurements of the longitudinal double-spin asymmetry, $A_{LL}$, for neutral pions produced at forward directions in polarized proton-proton collisions, at a center-of-mass energy of 510 GeV. Results are given for transverse momenta in the range $2
DOI: 10.17182/hepdata.98861.v1/t1
title: "Table 3: P-$\Omega$ correlation function" of "The Proton-$\Omega$ correlation function in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV"

description: Measured correlation function (C($k^{*}$)) for proton-$\Omega$ and antiproton-$\bar{\Omega}$ (P$\Omega$ + $\bar{P}$$\bar{\Omega}$) for (0-40)$\%$ and (40-80$\%$) Au+Au collisons at $\sqrt{s}_{NN}$ = 200 GeV. The errors are statistical and systematic.
description: 'We present the first measurement of the proton-$\Omega$ correlation function in heavy-ion collisions for central (0-40$\%$) and peripheral (40-80$\%$) Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV by the STAR experiment at the Relativistics Heavy-Ion Collider (RHIC). Predictions for the ratio of peripheral collisions to central collisons for the proton-$\Omega$ correlation function are sensitive to the presence of a nucleon-$\Omega$ bound state. These predictions are based on the proton-$\Omega$ interaction extracted from (2+1)-flavor lattice QCD calculations at the physical point. The measured ratio of proton-$\Omega$ correlation function from peripheral (small system) to central (large system) collisions is less than unity for relative momentum smaller than 40 MeV/c. Comparision of our measured correlation ratio with the theoretical calculation slightly favors a proton-$\Omega$ bound system with a binding energy of 27 MeV.'
DOI: 10.17182/hepdata.98861.v1/t2
title: "Table 4: Ratio of correlation function" of "The Proton-$\Omega$ correlation function in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV"

description: Ratio of small system (40-80$\%$) to large system (0-40$\%$) for proton-$\Omega$ and antiproton-$\bar{\Omega}$ (P$\Omega$ + $\bar{P}$$\Omega$). The errors are statistical and symmetric.
description: 'We present the first measurement of the proton-$\Omega$ correlation function in heavy-ion collisions for central (0-40$\%$) and peripheral (40-80$\%$) Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV by the STAR experiment at the Relativistics Heavy-Ion Collider (RHIC). Predictions for the ratio of peripheral collisions to central collisons for the proton-$\Omega$ correlation function are sensitive to the presence of a nucleon-$\Omega$ bound state. These predictions are based on the proton-$\Omega$ interaction extracted from (2+1)-flavor lattice QCD calculations at the physical point. The measured ratio of proton-$\Omega$ correlation function from peripheral (small system) to central (large system) collisions is less than unity for relative momentum smaller than 40 MeV/c. Comparision of our measured correlation ratio with the theoretical calculation slightly favors a proton-$\Omega$ bound system with a binding energy of 27 MeV.'
DOI: 10.17182/hepdata.166217.v1/t1
title: "Figure 2a" of "Combination of searches for heavy vector boson resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on the V'boson production cross section as functions of the resonance mass mV' shown separately for the V' → quarks category. The limits are evaluated in the HVT model A scenario.
description: A combined statistical analysis of searches for heavy vector boson resonances decaying into pairs of W, Z, or Higgs bosons, as well as into quark pairs (qqbar, bbbar, ttbar, tb) or lepton pairs (ellell, lnu), with l = e, mu, tau, is presented. The results are based on proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{-1}, collected by the CMS experiment from 2016 to 2018. No significant deviation from the expectations of the standard model is observed. The results are interpreted in the simplified heavy vector triplet (HVT) framework, setting 95% confidence level upper limits on the production cross sections and coupling strengths to standard model particles of the HVT bosons. The results exclude HVT resonances with masses below 5.5 TeV in a weakly coupled scenario, below 4.8 TeV in a strongly coupled scenario, and up to 2.0 TeV in the case of production via vector boson fusion. The combination provides the most stringent constraints to date on new phenomena predicted by the HVT model.
DOI: 10.17182/hepdata.166217.v1/t2
title: "Figure 2b" of "Combination of searches for heavy vector boson resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on the V'boson production cross section as functions of the resonance mass mV' shown separately for the V' → leptons category. The limits are evaluated in the HVT model A scenario.
description: A combined statistical analysis of searches for heavy vector boson resonances decaying into pairs of W, Z, or Higgs bosons, as well as into quark pairs (qqbar, bbbar, ttbar, tb) or lepton pairs (ellell, lnu), with l = e, mu, tau, is presented. The results are based on proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{-1}, collected by the CMS experiment from 2016 to 2018. No significant deviation from the expectations of the standard model is observed. The results are interpreted in the simplified heavy vector triplet (HVT) framework, setting 95% confidence level upper limits on the production cross sections and coupling strengths to standard model particles of the HVT bosons. The results exclude HVT resonances with masses below 5.5 TeV in a weakly coupled scenario, below 4.8 TeV in a strongly coupled scenario, and up to 2.0 TeV in the case of production via vector boson fusion. The combination provides the most stringent constraints to date on new phenomena predicted by the HVT model.
DOI: 10.17182/hepdata.166217.v1/t3
title: "Figure 3" of "Combination of searches for heavy vector boson resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on the V' boson production cross section as functions of the resonance mass mV' shown separately for the V' → bosons category. The limits are evaluated in the HVT model B scenario.
description: A combined statistical analysis of searches for heavy vector boson resonances decaying into pairs of W, Z, or Higgs bosons, as well as into quark pairs (qqbar, bbbar, ttbar, tb) or lepton pairs (ellell, lnu), with l = e, mu, tau, is presented. The results are based on proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{-1}, collected by the CMS experiment from 2016 to 2018. No significant deviation from the expectations of the standard model is observed. The results are interpreted in the simplified heavy vector triplet (HVT) framework, setting 95% confidence level upper limits on the production cross sections and coupling strengths to standard model particles of the HVT bosons. The results exclude HVT resonances with masses below 5.5 TeV in a weakly coupled scenario, below 4.8 TeV in a strongly coupled scenario, and up to 2.0 TeV in the case of production via vector boson fusion. The combination provides the most stringent constraints to date on new phenomena predicted by the HVT model.
DOI: 10.17182/hepdata.166217.v1/t5
title: "Figure 4b" of "Combination of searches for heavy vector boson resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on the V' boson production cross section as functions of the resonance mass mV' in the HVT model B.
description: A combined statistical analysis of searches for heavy vector boson resonances decaying into pairs of W, Z, or Higgs bosons, as well as into quark pairs (qqbar, bbbar, ttbar, tb) or lepton pairs (ellell, lnu), with l = e, mu, tau, is presented. The results are based on proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{-1}, collected by the CMS experiment from 2016 to 2018. No significant deviation from the expectations of the standard model is observed. The results are interpreted in the simplified heavy vector triplet (HVT) framework, setting 95% confidence level upper limits on the production cross sections and coupling strengths to standard model particles of the HVT bosons. The results exclude HVT resonances with masses below 5.5 TeV in a weakly coupled scenario, below 4.8 TeV in a strongly coupled scenario, and up to 2.0 TeV in the case of production via vector boson fusion. The combination provides the most stringent constraints to date on new phenomena predicted by the HVT model.
DOI: 10.17182/hepdata.166217.v1/t7
title: "Figure 6a" of "Combination of searches for heavy vector boson resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL exclusion contour in gF-gH parameter space for the DIQ channel at 3 TeV. Here, model A corresponds to (0.556, 0.562) and model B to (-2.928, 0.146)
description: A combined statistical analysis of searches for heavy vector boson resonances decaying into pairs of W, Z, or Higgs bosons, as well as into quark pairs (qqbar, bbbar, ttbar, tb) or lepton pairs (ellell, lnu), with l = e, mu, tau, is presented. The results are based on proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{-1}, collected by the CMS experiment from 2016 to 2018. No significant deviation from the expectations of the standard model is observed. The results are interpreted in the simplified heavy vector triplet (HVT) framework, setting 95% confidence level upper limits on the production cross sections and coupling strengths to standard model particles of the HVT bosons. The results exclude HVT resonances with masses below 5.5 TeV in a weakly coupled scenario, below 4.8 TeV in a strongly coupled scenario, and up to 2.0 TeV in the case of production via vector boson fusion. The combination provides the most stringent constraints to date on new phenomena predicted by the HVT model.
DOI: 10.17182/hepdata.166217.v1/t10
title: "Figure 6d" of "Combination of searches for heavy vector boson resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL exclusion contour in gF-gH parameter space for the DIL channel at 4 TeV.
description: A combined statistical analysis of searches for heavy vector boson resonances decaying into pairs of W, Z, or Higgs bosons, as well as into quark pairs (qqbar, bbbar, ttbar, tb) or lepton pairs (ellell, lnu), with l = e, mu, tau, is presented. The results are based on proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{-1}, collected by the CMS experiment from 2016 to 2018. No significant deviation from the expectations of the standard model is observed. The results are interpreted in the simplified heavy vector triplet (HVT) framework, setting 95% confidence level upper limits on the production cross sections and coupling strengths to standard model particles of the HVT bosons. The results exclude HVT resonances with masses below 5.5 TeV in a weakly coupled scenario, below 4.8 TeV in a strongly coupled scenario, and up to 2.0 TeV in the case of production via vector boson fusion. The combination provides the most stringent constraints to date on new phenomena predicted by the HVT model.