cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.46xvsk
title: Occurrence Download

description: A dataset containing 178 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Rhododendron farrerae Sweet",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 178 records from 9 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0267758-220831081235567/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.25921/gk4a-xt48
title: Water temperature, salinity, bathymetry, and sediment samples taken by CTD and multibeam sonar from the research vessel Ke Xue, cruise HOBAB5, in the North Pacific (Mariana trench) from 2018-06-07 to 2018-06-20 (NCEI Accession 0279921)

description: This dataset contains water temperature, salinity, bathymetry, sediment samples taken by CTD and the Sea Beam 3012 multibeam system from the research vessel Ke Xue, cruise HOBAB5, KEXUE-CN 20106443808. Bottom video recording is also included. This cruise is U.S. State Department MSR U2018-012 as part of the World Data Service for Geophysics and Oceanography. Processed CTD data are in CNV, raw CTD data are also included. Multibeam sonar data are in the Sea Beam 3012 format. Video is in MPEG format. Report is in PDF. Sediment analysis is described in publications listed in the Document section.
DOI: 10.17182/hepdata.82308.v1/t7
title: "Table 7" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Normalized dijet angular distribution for events with 2.4 &lt; dijet mass &lt; 3.0 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t10
title: "Table 10" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Electroweak correction factors for events with 5.4 &lt; dijet mass &lt; 6.0 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t11
title: "Table 11" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Electroweak correction factors for events with 4.8 &lt; dijet mass &lt; 5.4 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t12
title: "Table 12" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Electroweak correction factors for events with 4.2 &lt; dijet mass &lt; 4.8 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t13
title: "Table 13" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Electroweak correction factors for events with 3.6 &lt; dijet mass &lt; 4.2 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t14
title: "Table 14" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Electroweak correction factors for events with 3.0 &lt; dijet mass &lt; 3.6 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t15
title: "Table 15" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Electroweak correction factors for events with 2.4 &lt; dijet mass &lt; 3.0 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t8
title: "Table 8" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: The 95% CL upper limits on the quark coupling gq, as a function of mass, for an axialvector or vector DM mediator with gDM = 1.0 and mDM = 1 GeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t9
title: "Table 9" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Electroweak correction factors for events with dijet mass &gt; 6.0 TeV computed by the authors of JHEP 11 (2012) 095 (arXiv:1210.0438).
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t16
title: "Table 16" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 1 &lt; CHI &lt; 2.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t17
title: "Table 17" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 2 &lt; CHI &lt; 3.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t18
title: "Table 18" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 3 &lt; CHI &lt; 4.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t19
title: "Table 19" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 4 &lt; CHI &lt; 5.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t20
title: "Table 20" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 5 &lt; CHI &lt; 6.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t21
title: "Table 21" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 6 &lt; CHI &lt; 7.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t22
title: "Table 22" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 7 &lt; CHI &lt; 8.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t23
title: "Table 23" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 8 &lt; CHI &lt; 9.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t24
title: "Table 24" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 9 &lt; CHI &lt; 10.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t25
title: "Table 25" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 10 &lt; CHI &lt; 12.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t26
title: "Table 26" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 12 &lt; CHI &lt; 14.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t27
title: "Table 27" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: Covariance matrix for 14 &lt; CHI &lt; 16.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t28
title: "Table 28" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: NLO QCD+EW prediction and benchmark signal predictions for dijet mass &gt; 6.0 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t29
title: "Table 29" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: NLO QCD+EW prediction and benchmark signal predictions for 5.4 &lt; dijet mass &lt; 6.0 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t30
title: "Table 30" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: NLO QCD+EW prediction and benchmark signal predictions for 4.8 &lt; dijet mass &lt; 5.4 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t31
title: "Table 31" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: NLO QCD+EW prediction and benchmark signal predictions for 4.2 &lt; dijet mass &lt; 4.8 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t32
title: "Table 32" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: NLO QCD+EW prediction and benchmark signal predictions for 3.6 &lt; dijet mass &lt; 4.2 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t33
title: "Table 33" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: NLO QCD+EW prediction and benchmark signal predictions for 3.0 &lt; dijet mass &lt; 3.6 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82308.v1/t34
title: "Table 34" of "Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models"

description: NLO QCD+EW prediction and benchmark signal predictions for 2.4 &lt; dijet mass &lt; 3.0 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 35.9/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.82527.v1/t2
title: "Table 2: Cross-section limits gluon-gluon fusion" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The cross section times BR(A-&gt;ZH) times BR(H-&gt;bb) limits 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. The result refers to the nb=2 category only.
description: CERN-LHC. Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the llbb final state in pp collisions at sqrt(s)=13 TeV with the ATLAS detector. Data used 36 /fb. The final state contains electron-electron-b-b or muon-muon-b-b. A summary of the selection criteria is given in Table 1, page 6 of the preprint.
DOI: 10.17182/hepdata.82527.v1/t1
title: "Table 1: Signal Efficiency" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The signal efficiency for the production modes (gluon-gluon fusion and b-associated production) and the signal regions used in the analysis. The efficiency denominator has the total number of generated MC events. The numerator includes the events passing the full signal region selection, including the mbb window cuts. The table shows for each signal mass pair (mA, mH) 3 efficiencies corresponding to the two production modes in the two categories, 2tag and 3tag. These corresponds to "nb = 2 category" and "nb &gt;= 3 category", respectively, of the preprint. No numbers for gluon-gluon fusion in the 3tag category are provided since those are not used in the analysis. The efficiencies are given in fractions.
description: CERN-LHC. Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the llbb final state in pp collisions at sqrt(s)=13 TeV with the ATLAS detector. Data used 36 /fb. The final state contains electron-electron-b-b or muon-muon-b-b. A summary of the selection criteria is given in Table 1, page 6 of the preprint.
DOI: 10.17182/hepdata.82527.v1/t3
title: "Table 3: Cross-section limits b-associated production" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The cross section times BR(A-&gt;ZH) times BR(H-&gt;bb) limits for a narrow width A boson produced in association with b-quarks. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The result refers to the combination of the nb=2 and nb&gt;=3 categories.
description: CERN-LHC. Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the llbb final state in pp collisions at sqrt(s)=13 TeV with the ATLAS detector. Data used 36 /fb. The final state contains electron-electron-b-b or muon-muon-b-b. A summary of the selection criteria is given in Table 1, page 6 of the preprint.
DOI: 10.17182/hepdata.82527.v1/t4
title: "Table 4: Cross-section limits type-I tanb 1" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The cross section times BR(A-&gt;ZH) times BR(H-&gt;bb) limits for an A boson in the type-I, tanbeta 1, 2HDM. 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. For type-I only gluon-gluon fusion is used and the nb=2 category only.
description: CERN-LHC. Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the llbb final state in pp collisions at sqrt(s)=13 TeV with the ATLAS detector. Data used 36 /fb. The final state contains electron-electron-b-b or muon-muon-b-b. A summary of the selection criteria is given in Table 1, page 6 of the preprint.
DOI: 10.17182/hepdata.82527.v1/t5
title: "Table 5: Cross-section limits type-I tanb 5" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The cross section times BR(A-&gt;ZH) times BR(H-&gt;bb) limits for an A boson in the type-I, tanbeta 5, 2HDM. 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. For type-I only gluon-gluon fusion is used and the nb=2 category only.
description: CERN-LHC. Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the llbb final state in pp collisions at sqrt(s)=13 TeV with the ATLAS detector. Data used 36 /fb. The final state contains electron-electron-b-b or muon-muon-b-b. A summary of the selection criteria is given in Table 1, page 6 of the preprint.
DOI: 10.17182/hepdata.82527.v1/t6
title: "Table 6: Cross-section limits type-I tanb 10" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The cross section times BR(A-&gt;ZH) times BR(H-&gt;bb) limits for an A boson in the type-I, tanbeta 10, 2HDM. 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. For type-I only gluon-gluon fusion is used and the nb=2 category only.
description: CERN-LHC. Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the llbb final state in pp collisions at sqrt(s)=13 TeV with the ATLAS detector. Data used 36 /fb. The final state contains electron-electron-b-b or muon-muon-b-b. A summary of the selection criteria is given in Table 1, page 6 of the preprint.
DOI: 10.17182/hepdata.82527.v1/t7
title: "Table 7: Cross-section limits type-I tanb 20" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The cross section times BR(A-&gt;ZH) times BR(H-&gt;bb) limits for an A boson in the type-I, tanbeta 20, 2HDM. 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. For type-I only gluon-gluon fusion is used and the nb=2 category only.
description: CERN-LHC. Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the llbb final state in pp collisions at sqrt(s)=13 TeV with the ATLAS detector. Data used 36 /fb. The final state contains electron-electron-b-b or muon-muon-b-b. A summary of the selection criteria is given in Table 1, page 6 of the preprint.