cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95817.v1/t3
title: "fig15" of "High-pT pi^zero Production with Respect to the Reaction Plane in Au + Au Collisions at sqrt(s_NN) = 200 GeV"

description: Rebinned $R_{AA}$ for $\Delta \phi$, $p_T$, and path length dependence,
description: Measurements of the azimuthal anisotropy of high-$p_T$ neutral pion ($\pi^0$) production in Au+Au collisions at $\sqrt{sNN} = 200$ GeV by the PHENIX experiment are presented. The data included in this paper were collected during the 2004 RHIC running period and represent approximately an order of magnitude increase in the number of analyzed events relative to previously published results. Azimuthal angle distributions of $\pi^0$s detected in the PHENIX electromagnetic calorimeters are measured relative to the reaction plane determined event-by-event using the forward and backward beam-beam counters. Amplitudes of the second Fourier component ($v_2$) of the angular distributions are presented as a function of $\pi^0$ transverse momentum (pT) for different bins in collision centrality. Measured reaction plane dependent $\pi^0$ yields are used to determine the azimuthal dependence of the $\pi^0$ suppression as a function of pT, RAA(∆φ, pT). A jet-quenching motivated geometric analysis is presented that attempts to simultaneously describe the centrality dependence and reaction plane angle dependence of the $\pi^0$ suppression in terms of the path lengths of hypothetical parent partons 3 in the medium. This set of results allows for a detailed examination of the influence of geometry in the collision region, and of the interplay between collective flow and jet-quenching effects along the azimuthal axis.
DOI: 10.17182/hepdata.95817.v1/t4
title: "RAA vs dphi" of "High-pT pi^zero Production with Respect to the Reaction Plane in Au + Au Collisions at sqrt(s_NN) = 200 GeV"

description: Rebinned $R_{AA}$ for $\Delta \phi$, $p_T$, and path length dependence,
description: Measurements of the azimuthal anisotropy of high-$p_T$ neutral pion ($\pi^0$) production in Au+Au collisions at $\sqrt{sNN} = 200$ GeV by the PHENIX experiment are presented. The data included in this paper were collected during the 2004 RHIC running period and represent approximately an order of magnitude increase in the number of analyzed events relative to previously published results. Azimuthal angle distributions of $\pi^0$s detected in the PHENIX electromagnetic calorimeters are measured relative to the reaction plane determined event-by-event using the forward and backward beam-beam counters. Amplitudes of the second Fourier component ($v_2$) of the angular distributions are presented as a function of $\pi^0$ transverse momentum (pT) for different bins in collision centrality. Measured reaction plane dependent $\pi^0$ yields are used to determine the azimuthal dependence of the $\pi^0$ suppression as a function of pT, RAA(∆φ, pT). A jet-quenching motivated geometric analysis is presented that attempts to simultaneously describe the centrality dependence and reaction plane angle dependence of the $\pi^0$ suppression in terms of the path lengths of hypothetical parent partons 3 in the medium. This set of results allows for a detailed examination of the influence of geometry in the collision region, and of the interplay between collective flow and jet-quenching effects along the azimuthal axis.
DOI: 10.17182/hepdata.95826.v1/t1
title: "mbb in b-associated production, 2 tag" 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 bb system before any mbb window cuts for the 2 tag category in b-associated production. 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;bb) 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/t2
title: "mbb in b-associated production, 3 tag" 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 bb system before any mbb window cuts for the 3 tag category in b-associated production. 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;bb) 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/t3
title: "mllbb for gluon-gluon fusion, 2 tag, 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 mllbb mass distribution for the mbb window defined for (mA, mH)=(600, 300) GeV in the 2 tag category with gluon-gluon fusion production is shown. 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;bb) 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: 10.3535/1a3-4y9-vnb
title: Apera spica-venti (L.) P.Beauv.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/d9w-79l-gem
title: Spergula morisonii Boreau

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t4
title: "mllbb for b-associated production, 3 tag, 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 mllbb mass distribution for the mbb window defined for (mA, mH)=(600, 300) GeV in the 3 tag category with b-associated production is shown. 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;bb) 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/t5
title: "mllbb for gluon-gluon fusion, 2 tag, 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 mllbb mass distribution for the mbb window defined for (mA, mH)=(670, 500) GeV in the 2 tag category with gluon-gluon fusion production is shown. 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;bb) 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/t6
title: "mllbb for b-associated production, 3 tag, 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 mllbb mass distribution for the mbb window defined for (mA, mH) = (670, 500) GeV in the 3 tag category with b-associated production is shown. 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;bb) 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/t7
title: "Cross-section limits gluon-gluon fusion 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 a narrow width A boson produced via gluon-gluon fusion. 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/t8
title: "Cross-section limits b-associated production 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 a narrow width A boson produced via b-associated 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/t9
title: "Cross-section limits type 1 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 2HDM of type-1 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: 10.3535/2kx-0r2-b3e
title: Nardus stricta L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/wpc-pxs-k3n
title: Salix pentandra L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.95826.v1/t10
title: "Cross-section limits type 1 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 2HDM of type-1 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/t11
title: "Cross-section limits type 1 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 2HDM of type-1 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/t12
title: "Cross-section limits type 2 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 2HDM of type-2 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/t13
title: "Cross-section limits type 2 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 2HDM of type-2 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/t14
title: "Cross-section limits type 2 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 2HDM of type-2 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/t15
title: "Cross-section limits type 2 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 2HDM of type-2 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.