cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.103065.v1/t53
title: "Figure 11 Observed Lines" of "Search for top squark production in fully-hadronic final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The observed exclusion contour of the T5ttcc simplified model with respect to approximate NNLO+NNLL signal cross sections and the change in this contour due to variation of these cross sections within their theoretical uncertainties ($\sigma_{\text{theory}}$). The expected and observed upper limits do not take into account contributions from direct top squark pair production; however, its effect is small for $m_{\tilde{\chi}^0_1} &gt; 600 GeV$, which corresponds to the phase space beyond the exclusions based on direct top squark pair production. The excluded regions based on direct top squark pair production from this search and earlier searches are indicated by the hatched areas.
description: A search for production of the supersymmetric partners of the top quark, top squarks, is presented.The search is based on proton-proton collision events containing multiple jets, no leptons, and large transverse momentum imbalance.The data were collected with the CMS detector at the CERN LHC at a center-of-mass energy of 13 TeV, and correspond to an integrated luminosity of 137 $fb^-1$.The targeted signal production scenarios are direct and gluino-mediated top squark production, including scenarios in which the top squark and neutralino masses are nearly degenerate.The search utilizes novel algorithms based on deep neural networks that identify hadronically decaying top quarks and W bosons, which are expected in many of the targeted signal models.No statistically significant excess of events is observed relative to the expectation from the standard model, andlimits on the top squark production cross section are obtained in the context of simplified supersymmetric models for various production and decay modes.Exclusion limits as high as 1310 GeV are established at the 95% confidence level on the mass of the top squark for direct top squark production models,and as high as 2260 GeV on the mass of the gluino for gluino-mediated top squark production models.These results represent a significant improvement over the results of previous searches for supersymmetry by CMS in the same final state.
DOI: 10.17182/hepdata.103066.v1/t1
title: "Table 1" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Fitted values for the physical parameters of interest with their statistical and systematic uncertainties, for the result of solution (a).
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t2
title: "Table 2" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Fitted values for the physical parameters of interest with their statistical and systematic uncertainties, for the result of solution (b).
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t3
title: "Table 3" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Fit correlations between the physical parameters of interest, obtained from the fit for solution (a).
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t4
title: "Table 4" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Fit correlations between the physical parameters of interest, obtained from the fit for solution (b).
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t5
title: "Table 5" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Values of the physical parameters extracted in the combination of solution (a) of 13 TeV results with those obtained from 7 TeV and 8 TeV data.
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t6
title: "Table 6" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Values of the physical parameters extracted in the combination of solution (b) of 13 TeV results with those obtained from 7 TeV and 8 TeV data.
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t7
title: "Table 7" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Correlation matrix of the BLUE combination of the 7 TeV and 8 TeV results and the solution (a) of the 13 TeV result.
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t9
title: "Table 9" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Summary of systematic uncertainties assigned to the physical parameters of interest.
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103066.v1/t8
title: "Table 8" of "Measurement of the $CP$-violating phase $\phi_s$ in $B^0_s \to J/\psi\phi$ decays in ATLAS at 13 TeV"

description: Correlation matrix of the BLUE combination of the 7 TeV and 8 TeV results and the solution (b) of the 13 TeV result.
description: A measurement of the $B^0_s \to J/\psi\phi$ decay parameters using 80.5 $\mathrm{fb}^{-1}$ of integrated luminosity collected with the ATLAS detector from 13 TeV proton–proton collisions at the LHC is presented. The measured parameters include the $CP$-violating phase $\phi_s$, the width difference $\Delta\Gamma_{s}$ between the $B^0_s$ meson mass eigenstates and the average decay width $\Gamma_{s}$. The values measured for the physical parameters are combined with those from 19.2 $\mathrm{fb}^{-1}$ of 7 TeV and 8 TeV data, leading to the following:
\begin{eqnarray*}
\phi_s & = & -0.087\phantom{0} \pm 0.036\phantom{0} ~\mathrm{(stat.)} \pm 0.021\phantom{0} ~\mathrm{(syst.)~rad} \\
\Delta\Gamma_{s} & = & \phantom{-}0.0657 \pm 0.0043 ~\mathrm{(stat.)} \pm 0.0037 ~\mathrm{(syst.)~ps}^{-1} \\
\Gamma_{s} & = & \phantom{-}0.6703 \pm 0.0014 ~\mathrm{(stat.)} \pm 0.0018 ~\mathrm{(syst.)~ps}^{-1} \\
\end{eqnarray*}
Results for $\phi_s$ and $\Delta\Gamma_{s}$ are also presented as 68\% confidence level contours in the $\phi_s$--$\Delta\Gamma_{s}$ plane. Furthermore, the transversity amplitudes and corresponding strong phases are measured. $\phi_s$ and $\Delta\Gamma_{s}$ measurements are in agreement with the Standard Model predictions.
DOI: 10.17182/hepdata.103856.v1/t1
title: "Angular distribution" of "Search for heavy resonances decaying to Z($\nu\bar{\nu}$)V(q$\bar{q}$') in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Simulated distributions are shown for the cosine of the decay angle of SM vector bosons in the rest frame of a parent particle with a mass (mX) of 2\TeV. Solid lines represent VBF scenarios. Dashed lines represent ggF/DY scenarios.
description: A search is presented for heavy bosons decaying to Z($\nu\bar{\nu}$)V($q\bar{q'}$), where V can be a W or a Z boson. A sample of proton-proton collision data at $\sqrt{s}=13$ TeV was collected by the CMS experiment during 2016$-$2018.The data correspond to an integrated luminosity of $137 $\text{fb}^{-1}$. The event categorization is based on the presence of high-momentum jets in the forward region to identify production through weak vector boson fusion. Additional categorization uses jet substructure techniques andthe presence of large missing transverse momentum to identify W and Z bosons decaying to quarks and neutrinos, respectively.The dominant standard model backgrounds are estimated using data taken from control regions.The results are interpreted in terms of radion, W' boson, and graviton models, under the assumption that these bosons are produced via gluon-gluon fusion, Drell--Yan, or weak vector boson fusion processes. No evidence is found for physics beyond the standard model. Upper limits are set at 95\% confidence level on various types of hypothetical new bosons. Observed (expected) exclusion limits on the masses of these bosons range from 1.2 to 4.0 (1.1 to 3.7) TeV.
DOI: 10.17182/hepdata.103856.v1/t2
title: "mT shape for ggF-DY-produced resonance" of "Search for heavy resonances decaying to Z($\nu\bar{\nu}$)V(q$\bar{q}$') in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions of mT for ggF/DY-produced resonances X of mass 4.5 TeV.
description: A search is presented for heavy bosons decaying to Z($\nu\bar{\nu}$)V($q\bar{q'}$), where V can be a W or a Z boson. A sample of proton-proton collision data at $\sqrt{s}=13$ TeV was collected by the CMS experiment during 2016$-$2018.The data correspond to an integrated luminosity of $137 $\text{fb}^{-1}$. The event categorization is based on the presence of high-momentum jets in the forward region to identify production through weak vector boson fusion. Additional categorization uses jet substructure techniques andthe presence of large missing transverse momentum to identify W and Z bosons decaying to quarks and neutrinos, respectively.The dominant standard model backgrounds are estimated using data taken from control regions.The results are interpreted in terms of radion, W' boson, and graviton models, under the assumption that these bosons are produced via gluon-gluon fusion, Drell--Yan, or weak vector boson fusion processes. No evidence is found for physics beyond the standard model. Upper limits are set at 95\% confidence level on various types of hypothetical new bosons. Observed (expected) exclusion limits on the masses of these bosons range from 1.2 to 4.0 (1.1 to 3.7) TeV.
DOI: 10.17182/hepdata.103856.v1/t3
title: "mT shape for VBF-produced resonance" of "Search for heavy resonances decaying to Z($\nu\bar{\nu}$)V(q$\bar{q}$') in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions of mT for VBF-produced resonances X of mass 4.5 TeV.
description: A search is presented for heavy bosons decaying to Z($\nu\bar{\nu}$)V($q\bar{q'}$), where V can be a W or a Z boson. A sample of proton-proton collision data at $\sqrt{s}=13$ TeV was collected by the CMS experiment during 2016$-$2018.The data correspond to an integrated luminosity of $137 $\text{fb}^{-1}$. The event categorization is based on the presence of high-momentum jets in the forward region to identify production through weak vector boson fusion. Additional categorization uses jet substructure techniques andthe presence of large missing transverse momentum to identify W and Z bosons decaying to quarks and neutrinos, respectively.The dominant standard model backgrounds are estimated using data taken from control regions.The results are interpreted in terms of radion, W' boson, and graviton models, under the assumption that these bosons are produced via gluon-gluon fusion, Drell--Yan, or weak vector boson fusion processes. No evidence is found for physics beyond the standard model. Upper limits are set at 95\% confidence level on various types of hypothetical new bosons. Observed (expected) exclusion limits on the masses of these bosons range from 1.2 to 4.0 (1.1 to 3.7) TeV.
DOI: 10.17182/hepdata.103856.v1/t4
title: "Transfer factor for HP VBF category" of "Search for heavy resonances decaying to Z($\nu\bar{\nu}$)V(q$\bar{q}$') in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the transfer factor ($\alpha$) versus $m_T$ in the HP VBF category is shown. The last bin corresponds to the value obtained by integrating events above the penultimate bin.
description: A search is presented for heavy bosons decaying to Z($\nu\bar{\nu}$)V($q\bar{q'}$), where V can be a W or a Z boson. A sample of proton-proton collision data at $\sqrt{s}=13$ TeV was collected by the CMS experiment during 2016$-$2018.The data correspond to an integrated luminosity of $137 $\text{fb}^{-1}$. The event categorization is based on the presence of high-momentum jets in the forward region to identify production through weak vector boson fusion. Additional categorization uses jet substructure techniques andthe presence of large missing transverse momentum to identify W and Z bosons decaying to quarks and neutrinos, respectively.The dominant standard model backgrounds are estimated using data taken from control regions.The results are interpreted in terms of radion, W' boson, and graviton models, under the assumption that these bosons are produced via gluon-gluon fusion, Drell--Yan, or weak vector boson fusion processes. No evidence is found for physics beyond the standard model. Upper limits are set at 95\% confidence level on various types of hypothetical new bosons. Observed (expected) exclusion limits on the masses of these bosons range from 1.2 to 4.0 (1.1 to 3.7) TeV.
DOI: 10.17182/hepdata.103856.v1/t5
title: "Transfer factor for HP ggF-DY category" of "Search for heavy resonances decaying to Z($\nu\bar{\nu}$)V(q$\bar{q}$') in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of the transfer factor ($\alpha$) versus $m_T$ in the HP ggF/DY category is shown. The last bin corresponds to the value obtained by integrating events above the penultimate bin.
description: A search is presented for heavy bosons decaying to Z($\nu\bar{\nu}$)V($q\bar{q'}$), where V can be a W or a Z boson. A sample of proton-proton collision data at $\sqrt{s}=13$ TeV was collected by the CMS experiment during 2016$-$2018.The data correspond to an integrated luminosity of $137 $\text{fb}^{-1}$. The event categorization is based on the presence of high-momentum jets in the forward region to identify production through weak vector boson fusion. Additional categorization uses jet substructure techniques andthe presence of large missing transverse momentum to identify W and Z bosons decaying to quarks and neutrinos, respectively.The dominant standard model backgrounds are estimated using data taken from control regions.The results are interpreted in terms of radion, W' boson, and graviton models, under the assumption that these bosons are produced via gluon-gluon fusion, Drell--Yan, or weak vector boson fusion processes. No evidence is found for physics beyond the standard model. Upper limits are set at 95\% confidence level on various types of hypothetical new bosons. Observed (expected) exclusion limits on the masses of these bosons range from 1.2 to 4.0 (1.1 to 3.7) TeV.