cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.94263.v1/t3
title: "Cross-Sections" of "Results on Total and Elastic Cross Sections in Proton-Proton Collisions at $\sqrt{s} = 200$ GeV"

description: The total, elastic and inelastic cross-sections for proton-proton scattering at sqrt(s)=200 GeV, the elastic cross-section measured in the t-range 0.045&lt;|t|&lt;0.135 GeV^2 and the value of the differential cross-section extrapolated to |t| = 0.
description: We report results on the total and elastic cross sections in proton-proton collisions at $\sqrt{s}=200$~GeV obtained with the Roman Pot setup of the STAR experimentat the Relativistic Heavy Ion Collider (RHIC).The elastic differential cross section was measured in the squared four-momentum transfer range $0.045 \leq -t \leq 0.135$~GeV$^2$.The value of the exponential slope parameter $B$ of the elastic differential cross section $d\sigma/dt \sim e^{-Bt}$ in the measured $-t$ rangewas found to be $B = 14.32 \pm 0.09 (stat.)^{\scriptstyle +0.13}_{\scriptstyle -0.28} (syst.)$~GeV$^{-2}$. The total cross section $\sigma_{tot}$, obtained from extrapolation of the $d\sigma/dt$ to the optical point at $-t = 0$, is $\sigma_{tot} = 54.67 \pm 0.21 (stat.) ^{\scriptstyle +1.28}_{\scriptstyle -1.38} (syst.)$ mb.We also present the values of the elastic cross section $\sigma_{el} = 10.85 \pm 0.03 (stat.) ^{\scriptstyle +0.49}_{\scriptstyle -0.41}(syst.)$ mb,the elastic cross section integrated within the STAR $t$-range $\sigma^{det}_{el} = 4.05 \pm 0.01 (stat.) ^{\scriptstyle+0.18}_{\scriptstyle -0.17}(syst.)$ mb, and theinelastic cross section $\sigma_{inel} = 43.82 \pm 0.21 (stat.) ^{\scriptstyle +1.37}_{\scriptstyle -1.44} (syst.)$ mb.The results are compared with the world data.
DOI: 10.17182/hepdata.94264.v1/t47
title: "Table 5" of "Measurement of the central exclusive production of charged particle pairs in proton-proton collisions at $\sqrt{s} = 200$ GeV with the STAR detector at RHIC"

description: Exponential slope of the $t$-distribution in three ranges of $m(\pi^+\pi^-)$ and two ranges of $\Delta\varphi$.

The results are obtained for the Lorentz-invariant phase-space defined below:
 - $|y(\pi^+\pi^-)| &lt; 0.4$
 - $0.05~\mathrm{GeV}^2 &lt; -t_1, -t_2 &lt; 0.16~\mathrm{GeV}^2$
description: We report on the measurement of the Central Exclusive Production of charged particle pairs $h^{+}h^{-}$ ($h = \pi$, $K$, $p$) with the STAR detector at RHIC in proton-proton collisions at $\sqrt{s} = 200$ GeV. The charged particle pairs produced in the reaction $pp \to p^{\prime}+h^{+}h^{-}+p^{\prime}$ are reconstructed from the tracks in the central detector and identified using the specific energy loss and the time of flight method, while the forward-scattered protons are measured in the Roman Pot system. Exclusivity of the event is guaranteed by requiring the transverse momentum balance of all four final-state particles. Differential cross sections are measured as functions of observables related to the central hadronic final state and to the forward-scattered protons. They are measured in a fiducial region corresponding to the acceptance of the STAR detector and determined by the central particles' transverse momenta and pseudorapidities as well as by the forward-scattered protons' momenta. This fiducial region roughly corresponds to the square of the four-momentum transfers at the proton vertices in the range $0.04~\mathrm{GeV}^2 &lt; -t_1 , -t_2 &lt; 0.2~\mathrm{GeV}^2$, invariant masses of the charged particle pairs up to a few GeV and pseudorapidities of the centrally-produced hadrons in the range $|\eta|&lt;0.7$.The measured cross sections are compared to phenomenological predictions based on the Double Pomeron Exchange (DPE) model. Structures observed in the mass spectra of $\pi^{+}\pi^{-}$ and $K^{+}K^{-}$ pairs are consistent with the DPE model, while angular distributions of pions suggest a dominant spin-0 contribution to $\pi^{+}\pi^{-}$ production.For $\pi^+\pi^-$ production, the fiducial cross section is extrapolated to the Lorentz-invariant region, which allows decomposition of the invariant mass spectrum into continuum and resonant contributions. The extrapolated cross section is well described by the continuum production and at least three resonances, the $f_0(980)$, $f_2(1270)$ and $f_0(1500)$, with a possible small contribution from the $f_0(1370)$.Fits to the extrapolated differential cross section as a function of $t_1$ and $t_2$ enable extraction of the exponential slope parameters in several bins of the invariant mass of $\pi^+\pi^-$ pairs. These parameters are sensitive to the size of the interaction region.
DOI: 10.17182/hepdata.94286.v1/t1
title: "Table 1" of "Measurements of $\mathrm{t\bar{t}}$H production and the CP structure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel"

description: measured cross section times branch ratio
description: No data abstract available.
DOI: 10.17182/hepdata.94286.v1/t2
title: "Table 2" of "Measurements of $\mathrm{t\bar{t}}$H production and the CP structure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel"

description: measured cross section times branch divided by SM prediction
description: No data abstract available.
DOI: 10.17182/hepdata.94286.v1/t3
title: "Table 3" of "Measurements of $\mathrm{t\bar{t}}$H production and the CP structure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel"

description: Observed significance
description: No data abstract available.
DOI: 10.17182/hepdata.94286.v1/t4
title: "Table 4" of "Measurements of $\mathrm{t\bar{t}}$H production and the CP structure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel"

description: constraint on CP-odd contribution at 68% CL
description: No data abstract available.
DOI: 10.17182/hepdata.94286.v1/t5
title: "Table 5" of "Measurements of $\mathrm{t\bar{t}}$H production and the CP structure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel"

description: exclusion significance on pure CP odd contribution
description: No data abstract available.
DOI: 10.17182/hepdata.94288.v1/t1
title: "Figure 3 (left)" of "Measurement of the associated production of a Z boson with charm or bottom quark jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Unfolded R(c/j) cross section ratio versus jet transverse momentum
description: Ratios of cross sections, $\sigma(Z+\text{c jets})/\sigma(Z+\text{jets})$, $\sigma(Z+\text{b jets})/\sigma(Z+\text{jets})$, and $\sigma(Z+\text{c jets})/\sigma(Z+\text{b jets})$ in the associated production of a Z boson with at least one charm or bottom quark jet are measured in proton-proton collisions at $\sqrt s=13$ TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 $fb^{-1}$, with a fiducial volume of $p_T&gt;30$ GeV and $|\eta|&lt;2.4$ for the jets, where $p_T$ and $\eta$ represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with $p_T&gt;25$ GeV and $|\eta|&lt;2.4$, and the dilepton mass satisfies $71
DOI: 10.17182/hepdata.94288.v1/t2
title: "Figure 3 (right)" of "Measurement of the associated production of a Z boson with charm or bottom quark jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Unfolded R(c/j) cross section ratio versus Z boson transverse momentum
description: Ratios of cross sections, $\sigma(Z+\text{c jets})/\sigma(Z+\text{jets})$, $\sigma(Z+\text{b jets})/\sigma(Z+\text{jets})$, and $\sigma(Z+\text{c jets})/\sigma(Z+\text{b jets})$ in the associated production of a Z boson with at least one charm or bottom quark jet are measured in proton-proton collisions at $\sqrt s=13$ TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 $fb^{-1}$, with a fiducial volume of $p_T&gt;30$ GeV and $|\eta|&lt;2.4$ for the jets, where $p_T$ and $\eta$ represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with $p_T&gt;25$ GeV and $|\eta|&lt;2.4$, and the dilepton mass satisfies $71
DOI: 10.15468/dl.grm5pc
title: Occurrence Download

description: A dataset containing 21155 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-74.22848 40.49063,-74.22848 40.59637,-74.33385 40.59637,-74.33385 40.49063,-74.22848 40.49063))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Magnoliopsida"
 ]
}

 The dataset includes 21155 records from 37 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015786-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.94288.v1/t3
title: "Figure 4 (left)" of "Measurement of the associated production of a Z boson with charm or bottom quark jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Unfolded R(b/j) cross section ratio versus jet transverse momentum
description: Ratios of cross sections, $\sigma(Z+\text{c jets})/\sigma(Z+\text{jets})$, $\sigma(Z+\text{b jets})/\sigma(Z+\text{jets})$, and $\sigma(Z+\text{c jets})/\sigma(Z+\text{b jets})$ in the associated production of a Z boson with at least one charm or bottom quark jet are measured in proton-proton collisions at $\sqrt s=13$ TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 $fb^{-1}$, with a fiducial volume of $p_T&gt;30$ GeV and $|\eta|&lt;2.4$ for the jets, where $p_T$ and $\eta$ represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with $p_T&gt;25$ GeV and $|\eta|&lt;2.4$, and the dilepton mass satisfies $71
DOI: 10.17182/hepdata.94288.v1/t4
title: "Figure 4 (right)" of "Measurement of the associated production of a Z boson with charm or bottom quark jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Unfolded R(b/j) cross section ratio versus Z boson transverse momentum
description: Ratios of cross sections, $\sigma(Z+\text{c jets})/\sigma(Z+\text{jets})$, $\sigma(Z+\text{b jets})/\sigma(Z+\text{jets})$, and $\sigma(Z+\text{c jets})/\sigma(Z+\text{b jets})$ in the associated production of a Z boson with at least one charm or bottom quark jet are measured in proton-proton collisions at $\sqrt s=13$ TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 $fb^{-1}$, with a fiducial volume of $p_T&gt;30$ GeV and $|\eta|&lt;2.4$ for the jets, where $p_T$ and $\eta$ represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with $p_T&gt;25$ GeV and $|\eta|&lt;2.4$, and the dilepton mass satisfies $71
DOI: 10.17182/hepdata.94288.v1/t5
title: "Figure 5 (left)" of "Measurement of the associated production of a Z boson with charm or bottom quark jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Unfolded R(c/b) cross section ratio versus jet transverse momentum
description: Ratios of cross sections, $\sigma(Z+\text{c jets})/\sigma(Z+\text{jets})$, $\sigma(Z+\text{b jets})/\sigma(Z+\text{jets})$, and $\sigma(Z+\text{c jets})/\sigma(Z+\text{b jets})$ in the associated production of a Z boson with at least one charm or bottom quark jet are measured in proton-proton collisions at $\sqrt s=13$ TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 $fb^{-1}$, with a fiducial volume of $p_T&gt;30$ GeV and $|\eta|&lt;2.4$ for the jets, where $p_T$ and $\eta$ represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with $p_T&gt;25$ GeV and $|\eta|&lt;2.4$, and the dilepton mass satisfies $71
DOI: 10.17182/hepdata.94288.v1/t6
title: "Figure 5 (right)" of "Measurement of the associated production of a Z boson with charm or bottom quark jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Unfolded R(c/b) cross section ratio versus Z boson transverse momentum
description: Ratios of cross sections, $\sigma(Z+\text{c jets})/\sigma(Z+\text{jets})$, $\sigma(Z+\text{b jets})/\sigma(Z+\text{jets})$, and $\sigma(Z+\text{c jets})/\sigma(Z+\text{b jets})$ in the associated production of a Z boson with at least one charm or bottom quark jet are measured in proton-proton collisions at $\sqrt s=13$ TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of 35.9 $fb^{-1}$, with a fiducial volume of $p_T&gt;30$ GeV and $|\eta|&lt;2.4$ for the jets, where $p_T$ and $\eta$ represent transverse momentum and pseudorapidity, respectively. The Z boson candidates come from leptonic decays into electrons or muons with $p_T&gt;25$ GeV and $|\eta|&lt;2.4$, and the dilepton mass satisfies $71
DOI: 10.17182/hepdata.94311.v1/t1
title: "Table 04 - Yields Higgs Production Mode " of "Higgs boson production cross-section measurements and their EFT interpretation in the $4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The expected number of SM Higgs boson events with a mass $m_{H}$= 125 GeV for an integrated luminosity of 139 fb$^{-1}$ at $\sqrt{s}$=13 TeV in each reconstructed event signal (115 &lt; $m_{4l}$&lt; 130 GeV) and sideband ($m_{4l}$ in 105-115 GeV or 130-160 GeV for $ZZ^{*}$, 130-350 GeV for $tXX$) category, shown separately for each production bin of the Production Mode Stage. The ggF and $bbH$ yields are shown separately but both contribute to the same (ggF)production bin, and $ZH$ and $WH$ are reported separately but are merged together for the final result. Statistical and systematic uncertainties, including those for total SM cross-section predictions, are added in quadrature. Contributions that are below 0.2% of the total signal in each reconstructed event category are not shown and are replaced by -.
description: Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\mu$) using 139 fb$^{-1}$ of proton--proton collision data recorded at $\sqrt{s}$=13 TeV by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio for $H\to ZZ^*$ decay is measured to be $1.34 \pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd 'beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.
DOI: 10.17182/hepdata.94311.v1/t2
title: "Table 06 - Uncertainties" of "Higgs boson production cross-section measurements and their EFT interpretation in the $4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The impact of the dominant systematic uncertainties (in percent) on the cross-sections in production bins of the Production Mode Stage and the Reduced Stage 1.1. Similar sources of systematic uncertainties are grouped together in luminosity (Lumi.),electron/muon reconstruction and identification efficiencies and pile up modelling ($e$, $\mu$, pile up), jet energy scale/resolution and $b$-tagging efficiencies (Jets, flav. tag), uncertainties in reducible background (reducible bkg), theoretical uncertainties in $ZZ^{*}$ background and $tXX$ background, and theoretical uncertainties in the signal due to parton distribution function (PDF), QCD scale (QCD) and parton showering algorithm (Shower). The uncertainties are rounded to the nearest 0.5%, except for the luminosity uncertainty, which is measured to be 1.7% and increases for the $VH$ signal processes due to the simulation-based normalisation of the $VVV$ background. The uncertainties that are below 0.5% are not shown and replaced by -.
description: Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\mu$) using 139 fb$^{-1}$ of proton--proton collision data recorded at $\sqrt{s}$=13 TeV by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio for $H\to ZZ^*$ decay is measured to be $1.34 \pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd 'beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.
DOI: 10.17182/hepdata.94311.v1/t3
title: "Figure 05 - Distribution $m_{4l}$" of "Higgs boson production cross-section measurements and their EFT interpretation in the $4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The expected and the observed (post-fit) the four-lepton invariant mass distribution for the selected Higgs boson candidates, shown for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed tohave a mass $m_{H}$= 125GeV.
description: Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\mu$) using 139 fb$^{-1}$ of proton--proton collision data recorded at $\sqrt{s}$=13 TeV by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio for $H\to ZZ^*$ decay is measured to be $1.34 \pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd 'beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.
DOI: 10.17182/hepdata.94311.v1/t4
title: "Table 07 - Yields Results " of "Higgs boson production cross-section measurements and their EFT interpretation in the $4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The expected (pre-fit) and observed numbers of events for an integrated luminosity of 139 fb$^{-1}$ at $\sqrt{s}$=13 TeV in the signal region 115 &lt; $m_{4l}$&lt; 130 GeV and sideband region $m_{4l}$ in 105-115 GeV or 130-160 GeV (350 GeV for $tXX$-enriched) in each reconstructed event category assuming the SM Higgs boson signal with a mass $m_{H}$= 125 GeV. Combined statistical and systematic uncertainties are included for the predictions. Expected contributions that are below 0.2% of the total yield in each reconstructed event category are not shown and replaced by -.
description: Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\mu$) using 139 fb$^{-1}$ of proton--proton collision data recorded at $\sqrt{s}$=13 TeV by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio for $H\to ZZ^*$ decay is measured to be $1.34 \pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd 'beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.
DOI: 10.17182/hepdata.94311.v1/t5
title: "Figure 06a - Distribution $N_{jets}$" of "Higgs boson production cross-section measurements and their EFT interpretation in the $4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The expected and the observed (post-fit) the jet multiplicity distribution after the inclusive event selection for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.
description: Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\mu$) using 139 fb$^{-1}$ of proton--proton collision data recorded at $\sqrt{s}$=13 TeV by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio for $H\to ZZ^*$ decay is measured to be $1.34 \pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd 'beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.
DOI: 10.17182/hepdata.94311.v1/t6
title: "Figure 06b - Distribution $p_{T}^{4l}$ with $N_{jets}$=0" of "Higgs boson production cross-section measurements and their EFT interpretation in the $4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: The expected and the observed (post-fit) the four-lepton transverse momentum distribution for events with zero jets, after the inclusive event selection for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.
description: Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\mu$) using 139 fb$^{-1}$ of proton--proton collision data recorded at $\sqrt{s}$=13 TeV by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio for $H\to ZZ^*$ decay is measured to be $1.34 \pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd 'beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.