cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95826.v1/t16
title: "Cross-section limits lepton specific 2HDM tan(beta)=1 in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the total production cross-section (ggA + bbA) times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) for an A boson in the lepton specific 2HDM with tan(beta)=1. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used and cos(beta-alpha)=0 is assumed. The excluded contours in the figure correspond to the points of the 2HDM parameter space where the expected and observed limits match the theoretical prediction for the cross-section in the model.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.3535/rvw-vwv-myy
title: Corynephorus canescens (L.) P.Beauv.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t17
title: "Cross-section limits lepton specific 2HDM tan(beta)=2 in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the total production cross-section (ggA + bbA) times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) for an A boson in the lepton specific 2HDM with tan(beta)=2. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used and cos(beta-alpha)=0 is assumed. The excluded contours in the figure correspond to the points of the 2HDM parameter space where the expected and observed limits match the theoretical prediction for the cross-section in the model.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t18
title: "Cross-section limits lepton specific 2HDM tan(beta)=3 in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the total production cross-section (ggA + bbA) times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) for an A boson in the lepton specific 2HDM with tan(beta)=3. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used and cos(beta-alpha)=0 is assumed. The excluded contours in the figure correspond to the points of the 2HDM parameter space where the expected and observed limits match the theoretical prediction for the cross-section in the model.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t19
title: "Cross-section limits flipped 2HDM tan(beta)=1 in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the total production cross-section (ggA + bbA) times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) for an A boson in the flipped 2HDM with tan(beta)=1. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used and cos(beta-alpha)=0 is assumed. The excluded contours in the figure correspond to the points of the 2HDM parameter space where the expected and observed limits match the theoretical prediction for the cross-section in the model.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t20
title: "Cross-section limits flipped 2HDM tan(beta)=5 in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the total production cross-section (ggA + bbA) times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) for an A boson in the flipped 2HDM with tan(beta)=5. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used and cos(beta-alpha)=0 is assumed. The excluded contours in the figure correspond to the points of the 2HDM parameter space where the expected and observed limits match the theoretical prediction for the cross-section in the model.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t21
title: "Cross-section limits flipped 2HDM tan(beta)=10 in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the total production cross-section (ggA + bbA) times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) for an A boson in the flipped 2HDM with tan(beta)=10. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used and cos(beta-alpha)=0 is assumed. The excluded contours in the figure correspond to the points of the 2HDM parameter space where the expected and observed limits match the theoretical prediction for the cross-section in the model.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t22
title: "Cross-section limits flipped 2HDM tan(beta)=20 in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the total production cross-section (ggA + bbA) times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) for an A boson in the flipped 2HDM with tan(beta)=20. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used and cos(beta-alpha)=0 is assumed. The excluded contours in the figure correspond to the points of the 2HDM parameter space where the expected and observed limits match the theoretical prediction for the cross-section in the model.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t23
title: "m4q for gluon-gluon fusion, llWW" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The mass distribution of the 4q system before any m4q window cuts for gluon-gluon fusion for the llWW channel. The signal distribution for (mA, mH) = (600, 300) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.3535/6bb-dp7-mpc
title: Corylus avellana L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/p9g-0jh-n9y
title: Ulmus glabra Huds.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t24
title: "m2l4q for gluon-gluon fusion, llWW, mA 600 mH 300" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH)=(600, 300) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (600, 300) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t25
title: "m2l4q for gluon-gluon fusion, llWW, mA 670 mH 500" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The m2l4q mass distribution for the m4q window defined for (mA, mH)=(670, 500) GeV with gluon-gluon fusion production is shown for the llWW channel. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (670, 500) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A-&gt;ZH)xB(H-&gt;WW) corresponds to 1 pb. Background components are displayed separately.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t26
title: "Cross-section limits for llWW" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the production cross-section times the branching ratio B(A-&gt;ZH)xB(H-&gt;WW) in pb for a narrow width A boson produced via gluon-gluon fusion production. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t27
title: "Cross-section limits gluon-gluon fusion 10% width in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the production cross-section times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) in pb for an A boson with a natural width that is 10% with respect to its mass, produced via gluon-gluon fusion for the llbb final state. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t28
title: "Cross-section limits b-associated production 10% width in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the production cross-section times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) in pb for an A boson with a natural width that is 10% with respect to its mass, via b-associated production for the llbb final state. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t29
title: "Cross-section limits gluon-gluon fusion 20% width in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the production cross-section times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) in pb for an A boson with a natural width that is 20% with respect to its mass, produced via gluon-gluon fusion for the llbb final state. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.3535/wdd-wjy-66z
title: Ranunculus acris L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t30
title: "Cross-section limits b-associated production 20% width in llbb" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the production cross-section times the branching ratio B(A-&gt;ZH)xB(H-&gt;bb) in pb for an A boson with a natural width that is 20% with respect to its mass, via b-associated production for the llbb final state. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t31
title: "Cross-section limits gluon-gluon fusion 10% width in llWW" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the production cross-section times the branching ratio B(A-&gt;ZH)xB(H-&gt;WW) in pb for an A boson with a natural width that is 10% with respect to its mass, produced via gluon-gluon fusion for the llWW final state. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.
DOI: 10.17182/hepdata.95826.v1/t32
title: "Cross-section limits gluon-gluon fusion 20% width in llWW" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ and $\ell\ell WW$ final states in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Upper bounds at 95% CL on the production cross-section times the branching ratio B(A-&gt;ZH)xB(H-&gt;WW) in pb for an A boson with a natural width that is 20% with respect to its mass, produced via gluon-gluon fusion for the llWW final state. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected.
description: CERN-LHC. Search for a heavy Higgs boson, A, decaying into a Z boson and another heavy Higgs boson, H, in the llbb or llWW final state using a data sample corresponding to an integrated luminosity of 139/fb from proton-proton collisions at sqrt(s)=13 TeV recorded with the ATLAS detector. The final states contain electron-electron-b-b or muon-muon-b-b for llbb and electron-electron-4q or muon-muon-4q for llWW final states respectively. A summary of the selection criteria is given in Table 1, page 8 of the preprint.