cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83012.v1/t6
title: "Table 6" of "Search for heavy $ZZ$ resonances in the $\ell^+\ell^-\ell^+\ell^-$ and $\ell^+\ell^-\nu\bar\nu$ final states using proton proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance mass mH for the VBF production mode
description: CERN-LHC. Search for heavy ZZ resonances in the 4l and 2l2nu final states using proton-proton collisions at a center-of-mass energy of 13 TeV with 36.1 fb^{-1} of data collected during 2015 and 2016 with the ATLAS detector. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance.
DOI: 10.17182/hepdata.83012.v1/t7
title: "Table 7" of "Search for heavy $ZZ$ resonances in the $\ell^+\ell^-\ell^+\ell^-$ and $\ell^+\ell^-\nu\bar\nu$ final states using proton proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function of mH for an additioinal heavy scalar assuming a width of 1% of mH
description: CERN-LHC. Search for heavy ZZ resonances in the 4l and 2l2nu final states using proton-proton collisions at a center-of-mass energy of 13 TeV with 36.1 fb^{-1} of data collected during 2015 and 2016 with the ATLAS detector. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance.
DOI: 10.17182/hepdata.83012.v1/t8
title: "Table 8" of "Search for heavy $ZZ$ resonances in the $\ell^+\ell^-\ell^+\ell^-$ and $\ell^+\ell^-\nu\bar\nu$ final states using proton proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function of mH for an additioinal heavy scalar assuming a width of 5% of mH
description: CERN-LHC. Search for heavy ZZ resonances in the 4l and 2l2nu final states using proton-proton collisions at a center-of-mass energy of 13 TeV with 36.1 fb^{-1} of data collected during 2015 and 2016 with the ATLAS detector. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance.
DOI: 10.17182/hepdata.83012.v1/t10
title: "Table 10" of "Search for heavy $ZZ$ resonances in the $\ell^+\ell^-\ell^+\ell^-$ and $\ell^+\ell^-\nu\bar\nu$ final states using proton proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Upper limits at 95% CL on the cross section times branching ratio for a KK graviton produced with k/M_{PI} = 1.
description: CERN-LHC. Search for heavy ZZ resonances in the 4l and 2l2nu final states using proton-proton collisions at a center-of-mass energy of 13 TeV with 36.1 fb^{-1} of data collected during 2015 and 2016 with the ATLAS detector. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance.
DOI: 10.17182/hepdata.83012.v1/t9
title: "Table 9" of "Search for heavy $ZZ$ resonances in the $\ell^+\ell^-\ell^+\ell^-$ and $\ell^+\ell^-\nu\bar\nu$ final states using proton proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector"

description: Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function of mH for an additioinal heavy scalar assuming a width of 10% of mH
description: CERN-LHC. Search for heavy ZZ resonances in the 4l and 2l2nu final states using proton-proton collisions at a center-of-mass energy of 13 TeV with 36.1 fb^{-1} of data collected during 2015 and 2016 with the ATLAS detector. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance.
DOI: 10.17182/hepdata.83104.v1/t1
title: "Table 0: Final Variable Distribution (RECOSR)" of "Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The hadronically decaying VLB candidate mass in the RECOSR region after the maximum likelihood fit in the two signal regions overlayed with the pre-fit VLB signal
description: CERN-LHC, ATLAS. Limits on pair production of a heavy vector-like B quark together with its antiparticle, where the B quark decays to a W boson and a top quark. The search is based on 36.1 +\- 0.8 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the lepton plus jets final state, including at least four small jets out of which at least one is required to be b-tagged jet and a large-radius jet. Mass limits on B production are set as a function of the decay branching ratios. 

Basic event selection:
- ==1 electron or muon: pT &gt;= 30 GeV, in fiducial volume, isolated from jets
- Missing transverse momentum &gt;= 60 GeV
- &gt;=4 small-R jets, with at least one b-tagged
- &gt;=1 large-radius jet
- S_T &gt; 1200 GeV
 Comment: Leptonically and hadronically decaying VLQ candidates are reconstructed (see paper) .

Additional selection:
 Signal region 1 (RECOSR):
 - &gt;=3 large-radius jets
 - &gt;=1 hadronic W candidate: W-tagged large-R jet not overlapping with a b-tagged jet
 - S_T &gt;= 1500 GeV
 - Delta R(lepton, p_T leading b-jet) &gt;= 1
 Comment: Final discriminant is the mass of the hadronically decaying VLB candidate

 Signal region 2 (BDTSR):
 - S_T &gt;= 1200 GeV 
 - RECOSR veto 
 Comment: Final discriminant is the BDT discriminant
DOI: 10.17182/hepdata.83104.v1/t2
title: "Table 1: Final Variable Distribution (BDTSR)" of "Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The BDT discriminant in the BDTSR region after the maximum likelihood fit in the two signal regions overlayed with the pre-fit VLB signal
description: CERN-LHC, ATLAS. Limits on pair production of a heavy vector-like B quark together with its antiparticle, where the B quark decays to a W boson and a top quark. The search is based on 36.1 +\- 0.8 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the lepton plus jets final state, including at least four small jets out of which at least one is required to be b-tagged jet and a large-radius jet. Mass limits on B production are set as a function of the decay branching ratios. 

Basic event selection:
- ==1 electron or muon: pT &gt;= 30 GeV, in fiducial volume, isolated from jets
- Missing transverse momentum &gt;= 60 GeV
- &gt;=4 small-R jets, with at least one b-tagged
- &gt;=1 large-radius jet
- S_T &gt; 1200 GeV
 Comment: Leptonically and hadronically decaying VLQ candidates are reconstructed (see paper) .

Additional selection:
 Signal region 1 (RECOSR):
 - &gt;=3 large-radius jets
 - &gt;=1 hadronic W candidate: W-tagged large-R jet not overlapping with a b-tagged jet
 - S_T &gt;= 1500 GeV
 - Delta R(lepton, p_T leading b-jet) &gt;= 1
 Comment: Final discriminant is the mass of the hadronically decaying VLB candidate

 Signal region 2 (BDTSR):
 - S_T &gt;= 1200 GeV 
 - RECOSR veto 
 Comment: Final discriminant is the BDT discriminant
DOI: 10.17182/hepdata.83104.v1/t3
title: "Table 2: BB-&gt;WtWt Cross Section Limit" of "Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Expected and observed upper limits at the 95% CL on the BB cross section as a function of B quark mass under the assumption of BR(B-&gt;Wt)=1.
description: CERN-LHC, ATLAS. Limits on pair production of a heavy vector-like B quark together with its antiparticle, where the B quark decays to a W boson and a top quark. The search is based on 36.1 +\- 0.8 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the lepton plus jets final state, including at least four small jets out of which at least one is required to be b-tagged jet and a large-radius jet. Mass limits on B production are set as a function of the decay branching ratios. 

Basic event selection:
- ==1 electron or muon: pT &gt;= 30 GeV, in fiducial volume, isolated from jets
- Missing transverse momentum &gt;= 60 GeV
- &gt;=4 small-R jets, with at least one b-tagged
- &gt;=1 large-radius jet
- S_T &gt; 1200 GeV
 Comment: Leptonically and hadronically decaying VLQ candidates are reconstructed (see paper) .

Additional selection:
 Signal region 1 (RECOSR):
 - &gt;=3 large-radius jets
 - &gt;=1 hadronic W candidate: W-tagged large-R jet not overlapping with a b-tagged jet
 - S_T &gt;= 1500 GeV
 - Delta R(lepton, p_T leading b-jet) &gt;= 1
 Comment: Final discriminant is the mass of the hadronically decaying VLB candidate

 Signal region 2 (BDTSR):
 - S_T &gt;= 1200 GeV 
 - RECOSR veto 
 Comment: Final discriminant is the BDT discriminant
DOI: 10.17182/hepdata.83104.v1/t4
title: "Table 3: SU(2) Singlet Cross Section Limit" of "Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Expected and observed upper limits at the 95% CL on the BB cross section as a function of B quark mass in the SU(2) singlet scenario.
description: CERN-LHC, ATLAS. Limits on pair production of a heavy vector-like B quark together with its antiparticle, where the B quark decays to a W boson and a top quark. The search is based on 36.1 +\- 0.8 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the lepton plus jets final state, including at least four small jets out of which at least one is required to be b-tagged jet and a large-radius jet. Mass limits on B production are set as a function of the decay branching ratios. 

Basic event selection:
- ==1 electron or muon: pT &gt;= 30 GeV, in fiducial volume, isolated from jets
- Missing transverse momentum &gt;= 60 GeV
- &gt;=4 small-R jets, with at least one b-tagged
- &gt;=1 large-radius jet
- S_T &gt; 1200 GeV
 Comment: Leptonically and hadronically decaying VLQ candidates are reconstructed (see paper) .

Additional selection:
 Signal region 1 (RECOSR):
 - &gt;=3 large-radius jets
 - &gt;=1 hadronic W candidate: W-tagged large-R jet not overlapping with a b-tagged jet
 - S_T &gt;= 1500 GeV
 - Delta R(lepton, p_T leading b-jet) &gt;= 1
 Comment: Final discriminant is the mass of the hadronically decaying VLB candidate

 Signal region 2 (BDTSR):
 - S_T &gt;= 1200 GeV 
 - RECOSR veto 
 Comment: Final discriminant is the BDT discriminant
DOI: 10.17182/hepdata.83104.v1/t5
title: "Table 4: Limit on B mass vs. BR" of "Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Expected and observed 95% CL lower limits on the mass of the B quark in the branching ratio plane of BR(B-&gt;Wt) versus BR(B-&gt;Hb).
description: CERN-LHC, ATLAS. Limits on pair production of a heavy vector-like B quark together with its antiparticle, where the B quark decays to a W boson and a top quark. The search is based on 36.1 +\- 0.8 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the lepton plus jets final state, including at least four small jets out of which at least one is required to be b-tagged jet and a large-radius jet. Mass limits on B production are set as a function of the decay branching ratios. 

Basic event selection:
- ==1 electron or muon: pT &gt;= 30 GeV, in fiducial volume, isolated from jets
- Missing transverse momentum &gt;= 60 GeV
- &gt;=4 small-R jets, with at least one b-tagged
- &gt;=1 large-radius jet
- S_T &gt; 1200 GeV
 Comment: Leptonically and hadronically decaying VLQ candidates are reconstructed (see paper) .

Additional selection:
 Signal region 1 (RECOSR):
 - &gt;=3 large-radius jets
 - &gt;=1 hadronic W candidate: W-tagged large-R jet not overlapping with a b-tagged jet
 - S_T &gt;= 1500 GeV
 - Delta R(lepton, p_T leading b-jet) &gt;= 1
 Comment: Final discriminant is the mass of the hadronically decaying VLB candidate

 Signal region 2 (BDTSR):
 - S_T &gt;= 1200 GeV 
 - RECOSR veto 
 Comment: Final discriminant is the BDT discriminant
DOI: 10.17182/hepdata.83155.v1/t1
title: "Table 0" of "Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Expected and observed 95% CL upper limits for the production of a single narrow resonance, $\phi$, with a mass between 90 GeV and 3.2 TeV via gluon-gluon fusion. This limit database corresponds to the values shown in Figure 7a of the paper.
description: A search is presented for additional neutral Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at the LHC. The search is performed in the context of the minimal supersymmetric extension of the standard model (MSSM), using the data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes production of the Higgs boson in association with b quarks. No significant deviation above the expected background is observed. Model-independent limits at 95% confidence level (CL) are set on the product of the branching fraction for the decay into $\tau$ leptons and the cross section for the production via gluon fusion or in association with b quarks. These limits range from 18 pb at 90 GeV to 3.5 fb at 3.2 TeV for gluon fusion and from 15 pb (at 90 GeV) to 2.5 fb (at 3.2 TeV) for production in association with b quarks. In the m$_{\text{h}}^{\text{mod+}}$ scenario these limits translate into a 95% CL exclusion of $\tan\beta&gt;$ 6 for neutral Higgs boson masses below 250 GeV, where $\tan\beta$ is the ratio of the vacuum expectation values of the neutral components of the two Higgs doublets. The 95% CL exclusion contour reaches 1.6 TeV for $\tan\beta=$ 60.
DOI: 10.17182/hepdata.83155.v1/t2
title: "Table 1" of "Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Expected and observed 95% CL upper limits for the production of a single narrow resonance, $\phi$, with a mass between 90 GeV and 3.2 TeV in association with b-quarks. This limit database corresponds to the values shown in Figure 7b of the paper.
description: A search is presented for additional neutral Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at the LHC. The search is performed in the context of the minimal supersymmetric extension of the standard model (MSSM), using the data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes production of the Higgs boson in association with b quarks. No significant deviation above the expected background is observed. Model-independent limits at 95% confidence level (CL) are set on the product of the branching fraction for the decay into $\tau$ leptons and the cross section for the production via gluon fusion or in association with b quarks. These limits range from 18 pb at 90 GeV to 3.5 fb at 3.2 TeV for gluon fusion and from 15 pb (at 90 GeV) to 2.5 fb (at 3.2 TeV) for production in association with b quarks. In the m$_{\text{h}}^{\text{mod+}}$ scenario these limits translate into a 95% CL exclusion of $\tan\beta&gt;$ 6 for neutral Higgs boson masses below 250 GeV, where $\tan\beta$ is the ratio of the vacuum expectation values of the neutral components of the two Higgs doublets. The 95% CL exclusion contour reaches 1.6 TeV for $\tan\beta=$ 60.
DOI: 10.17182/hepdata.83155.v1/t3
title: "Table 2" of "Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Scan of the likelihood function for the search in the $\tau\tau$ final state for a single narrow resonance, $\phi$, produced via gluon fusion ($gg\phi$) or in association with b quarks ($bb\phi$). The scan is performed in 40000 points of the ($\sigma(gg\phi)\cdot B(\phi\rightarrow\tau\tau)$, $\sigma(bb\phi)\cdot B(\phi\rightarrow\tau\tau)$) plane. An asimov dataset constructed from the expectation of all backgrounds and the SM Higgs boson is tested against a background hypothesis including the SM Higgs boson. For further details and instructions, please have a look into the following README file http://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-17-020/2D-likelihood-scans/README.txt. Selected examples of such a likelihood scan are given in Figure 8 of the paper.
description: A search is presented for additional neutral Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at the LHC. The search is performed in the context of the minimal supersymmetric extension of the standard model (MSSM), using the data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes production of the Higgs boson in association with b quarks. No significant deviation above the expected background is observed. Model-independent limits at 95% confidence level (CL) are set on the product of the branching fraction for the decay into $\tau$ leptons and the cross section for the production via gluon fusion or in association with b quarks. These limits range from 18 pb at 90 GeV to 3.5 fb at 3.2 TeV for gluon fusion and from 15 pb (at 90 GeV) to 2.5 fb (at 3.2 TeV) for production in association with b quarks. In the m$_{\text{h}}^{\text{mod+}}$ scenario these limits translate into a 95% CL exclusion of $\tan\beta&gt;$ 6 for neutral Higgs boson masses below 250 GeV, where $\tan\beta$ is the ratio of the vacuum expectation values of the neutral components of the two Higgs doublets. The 95% CL exclusion contour reaches 1.6 TeV for $\tan\beta=$ 60.
DOI: 10.17182/hepdata.83155.v1/t4
title: "Table 3" of "Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Scan of the likelihood function for the search in the $\tau\tau$ final state for a single narrow resonance, $\phi$, produced via gluon fusion ($gg\phi$) or in association with b quarks ($bb\phi$). The scan is performed in 40000 points of the ($\sigma(gg\phi)\cdot B(\phi\rightarrow\tau\tau)$, $\sigma(bb\phi)\cdot B(\phi\rightarrow\tau\tau)$) plane. An asimov dataset constructed from the expectation of all backgrounds is tested against a background hypothesis without the SM Higgs boson. For further details and instructions, please have a look into the following README file http://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-17-020/2D-likelihood-scans/README.txt. Selected examples of such a likelihood scan are given in Figure 8 of the paper.
description: A search is presented for additional neutral Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at the LHC. The search is performed in the context of the minimal supersymmetric extension of the standard model (MSSM), using the data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes production of the Higgs boson in association with b quarks. No significant deviation above the expected background is observed. Model-independent limits at 95% confidence level (CL) are set on the product of the branching fraction for the decay into $\tau$ leptons and the cross section for the production via gluon fusion or in association with b quarks. These limits range from 18 pb at 90 GeV to 3.5 fb at 3.2 TeV for gluon fusion and from 15 pb (at 90 GeV) to 2.5 fb (at 3.2 TeV) for production in association with b quarks. In the m$_{\text{h}}^{\text{mod+}}$ scenario these limits translate into a 95% CL exclusion of $\tan\beta&gt;$ 6 for neutral Higgs boson masses below 250 GeV, where $\tan\beta$ is the ratio of the vacuum expectation values of the neutral components of the two Higgs doublets. The 95% CL exclusion contour reaches 1.6 TeV for $\tan\beta=$ 60.
DOI: 10.17182/hepdata.83155.v1/t5
title: "Table 4" of "Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Scan of the likelihood function for the search in the $\tau\tau$ final state for a single narrow resonance, $\phi$, produced via gluon fusion ($gg\phi$) or in association with b quarks ($bb\phi$). The scan is performed in 40000 points of the ($\sigma(gg\phi)\cdot B(\phi\rightarrow\tau\tau)$, $\sigma(bb\phi)\cdot B(\phi\rightarrow\tau\tau)$) plane. The observation in data is tested against a background hypothesis including the SM Higgs boson. For further details and instructions, please have a look into the following README file http://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-17-020/2D-likelihood-scans/README.txt. Selected examples of such a likelihood scan are given in Figure 8 of the paper.
description: A search is presented for additional neutral Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at the LHC. The search is performed in the context of the minimal supersymmetric extension of the standard model (MSSM), using the data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes production of the Higgs boson in association with b quarks. No significant deviation above the expected background is observed. Model-independent limits at 95% confidence level (CL) are set on the product of the branching fraction for the decay into $\tau$ leptons and the cross section for the production via gluon fusion or in association with b quarks. These limits range from 18 pb at 90 GeV to 3.5 fb at 3.2 TeV for gluon fusion and from 15 pb (at 90 GeV) to 2.5 fb (at 3.2 TeV) for production in association with b quarks. In the m$_{\text{h}}^{\text{mod+}}$ scenario these limits translate into a 95% CL exclusion of $\tan\beta&gt;$ 6 for neutral Higgs boson masses below 250 GeV, where $\tan\beta$ is the ratio of the vacuum expectation values of the neutral components of the two Higgs doublets. The 95% CL exclusion contour reaches 1.6 TeV for $\tan\beta=$ 60.