cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.155471.v1/t25
title: "Figure 8(3)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2017 analysis in the SL category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t26
title: "Figure 9(1)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2017 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t27
title: "Figure 9(2)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2017 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t28
title: "Figure 9(3)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2017 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t29
title: "Figure 9(4)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2017 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t30
title: "Figure 10(1)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2018 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t31
title: "Figure 10(2)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2018 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t32
title: "Figure 10(3)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2018 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.17182/hepdata.155471.v1/t33
title: "Figure 10(4)" of "Search for bosons of an extended Higgs sector in b quark final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Background-only fits to the M12 distribution in each fit range of the 2018 analysis in the FH category
description: A search for beyond-the-standard-model neutral Higgs bosons in final states with bottom quarks is performed with the CMS detector. The data analysed were recorded in proton-proton collisions at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of up to 36.7-126.9 $fb^{-1}$. No signal above the standard model background expectation is observed. Stringent upper limits on the cross section times branching fraction are set for Higgs bosons in the mass range of 125-1800 GeV. The results are interpreted in benchmark scenarios of the minimal supersymmetric standard model, as well as suitable classes of two Higgs doublet models.
DOI: 10.15468/dl.pyet36
title: Occurrence Download

description: A dataset containing 39207260 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Aves)",
 "Country is one of (Brazil, Argentina, Paraguay)",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 {
 "not" : {
 "BasisOfRecord" : [
 "is Fossil"
 ]
 }
 },
 {
 "not" : {
 "OccurrenceStatus" : [
 "is Absent"
 ]
 }
 }
 ]
}

 The dataset includes 39207260 records from 221 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015982-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.155497.v1/t1
title: "Table 1" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Summary of results in terms of best fit value of the Wilson coefficients and the intervals where the test statistic is below 1 and 4, with up to the linear and quadratic terms in the SMEFT parameterization.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t2
title: "Table 2" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Profiled limits on the energy scale $\Lambda$ for three different assumptions for each Wilson coefficient while fixing the other Wilson coefficients to their SM values with up to the linear and quadratic terms in SMEFT parameterization.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t3
title: "Table 9a" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $c_{Hq}^{(3)}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t4
title: "Table 9b" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $c_{Hq}^{(3)}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t5
title: "Table 9c" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $c_{Hu}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t6
title: "Table 9d" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $c_{Hu}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t7
title: "Table 9e" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $c_{Hd}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t8
title: "Table 9f" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $c_{Hd}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t9
title: "Table 10a" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $c_{Hu}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t10
title: "Table 10b" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $c_{Hu}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t11
title: "Table 10c" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $c_{Hd}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t12
title: "Table 10d" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $c_{Hd}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t13
title: "Table 10e" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hu}$ vs. $c_{Hd}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t14
title: "Table 10f" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hu}$ vs. $c_{Hd}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t15
title: "Table 11a" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $g^{(2)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t16
title: "Table 11b" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $g^{(2)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t17
title: "Table 11c" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $g^{(2)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t18
title: "Table 11d" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $g^{(2)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t19
title: "Table 11e" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hu}$ vs. $g^{(2)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t20
title: "Table 11f" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hu}$ vs. $g^{(2)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t21
title: "Table 12a" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $g^{(4)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t22
title: "Table 12b" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(1)}$ vs. $g^{(4)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t23
title: "Table 12c" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $g^{(4)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t24
title: "Table 12d" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hq}^{(3)}$ vs. $g^{(4)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t25
title: "Table 112e" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hu}$ vs. $g^{(4)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t26
title: "Table 12f" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hu}$ vs. $g^{(4)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t27
title: "Table 13a" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hd}$ vs. $g^{(2)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t28
title: "Table 13b" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hd}$ vs. $g^{(2)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t29
title: "Table 13c" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hd}$ vs. $g^{(4)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t30
title: "Table 13d" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $c_{Hd}$ vs. $g^{(4)}_{ZZ}$ while other coefficients are fixed at their SM values.
description: No data abstract available.
DOI: 10.17182/hepdata.155497.v1/t31
title: "Table 13e" of "Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H$\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed two-dimensional likelihood scans for $g^{(2)}_{ZZ}$ vs. $g^{(4)}_{ZZ}$ while allowing the other coefficients to float freely at each point of the sca.
description: No data abstract available.