cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95826.v1/t157
title: "m2l4q for gluon-gluon fusion, llWW, mA 550 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) = (550, 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) = (550, 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/t158
title: "m2l4q for gluon-gluon fusion, llWW, mA 550 mH 310" 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) = (550, 310) 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) = (550, 310) 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/t159
title: "m2l4q for gluon-gluon fusion, llWW, mA 560 mH 320" 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) = (560, 320) 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) = (560, 320) 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/t160
title: "m2l4q for gluon-gluon fusion, llWW, mA 570 mH 330" 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) = (570, 330) 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) = (570, 330) 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/t161
title: "m2l4q for gluon-gluon fusion, llWW, mA 570 mH 340" 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) = (570, 340) 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) = (570, 340) 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/t162
title: "m2l4q for gluon-gluon fusion, llWW, mA 580 mH 350" 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) = (580, 350) 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) = (580, 350) 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/t163
title: "m2l4q for gluon-gluon fusion, llWW, mA 580 mH 360" 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) = (580, 360) 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) = (580, 360) 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/t164
title: "m2l4q for gluon-gluon fusion, llWW, mA 590 mH 370" 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) = (590, 370) 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) = (590, 370) 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: 10.3535/5e6-bz3-pvv
title: Helichrysum arenarium (L.) Moench

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/gbw-z8x-gzn
title: Convallaria majalis L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t165
title: "m2l4q for gluon-gluon fusion, llWW, mA 600 mH 380" 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, 380) 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, 380) 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/t166
title: "m2l4q for gluon-gluon fusion, llWW, mA 600 mH 390" 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, 390) 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, 390) 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/t167
title: "m2l4q for gluon-gluon fusion, llWW, mA 610 mH 400" 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) = (610, 400) 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) = (610, 400) 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/t168
title: "m2l4q for gluon-gluon fusion, llWW, mA 620 mH 410" 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) = (620, 410) 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) = (620, 410) 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/t169
title: "m2l4q for gluon-gluon fusion, llWW, mA 620 mH 420" 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) = (620, 420) 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) = (620, 420) 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/t170
title: "m2l4q for gluon-gluon fusion, llWW, mA 630 mH 430" 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) = (630, 430) 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) = (630, 430) 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/t171
title: "m2l4q for gluon-gluon fusion, llWW, mA 630 mH 440" 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) = (630, 440) 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) = (630, 440) 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/t172
title: "m2l4q for gluon-gluon fusion, llWW, mA 640 mH 450" 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) = (640, 450) 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) = (640, 450) 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/t173
title: "m2l4q for gluon-gluon fusion, llWW, mA 650 mH 460" 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) = (650, 460) 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) = (650, 460) 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/g6q-pmn-hna
title: Ajuga reptans L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.