cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.5281/zenodo.17338021
title: Data from: Soluble Iron Deposition Shifts External Nitrogen Supply in Oligotrophic Oceans

description: Decadal external nitrogen supply fields from the study "Soluble Iron Deposition Shifts External Nitrogen Supply in Oligotrophic Gyres" are provided here.

The dataset contains gridded (2° latitude × 2.5° longitude) fields for the 1980s, 1990s, 2000s, and 2010s, including:

NFIX: Decadal mean nitrogen fixation rates (mmol N m⁻² yr⁻¹) estimated from CESM2-derived soluble iron deposition and GEOS-Chem-derived inorganic nitrogen deposition.NFIXadj: Adjusted decadal mean nitrogen fixation rates (mmol N m⁻² yr⁻¹) considering nutrient co-limitation of phosphorus and iron on NFIX.NDEP: Decadal mean inorganic nitrogen deposition rates (mmol N m⁻² yr⁻¹) from GEOS-Chem simulations.NVER: Climatological vertical nitrogen supply (mmol N m⁻² yr⁻¹) calculated based on GLODAPv2 nitrate concentration.EP: Decadal mean export production at 100 m depth based on CESM2-POP2 particulate organic carbon flux (g C m⁻² yr⁻¹).NPP: Climatological net primary production (g C m⁻² yr⁻¹) from VGPM and CbPM2 satellite-based products.

Decades are represented by the central year of each period (1985, 1995, 2005, 2015). All data fields follow CF-1.9 conventions.

Acknowledgments

M.-W.S. and T.-W.K. were supported by the National Research Foundation of Korea (Grant Nos. RS-2024-00337227, RS-2022-NR068504), and by the BK21 FOUR program (Grant No. 4120200313708). Additional support for T.-W.K. was provided by the OJEong Resilience Institute, Korea University. N.M.M., and L.L. were supported by the U.S. Department of Energy (DOE) under Grant No. DE-SC0021302, and the Earth Surface Mineral Dust Source InvesTigation (EMIT), a NASA Earth Ventures-Instrument (EVI-4) Mission.
DOI: 10.17182/hepdata.142374.v1/t5
title: "Figure 3b" of "Measurement of identified pi0 and inclusive photon v(2) and implication to the direct photon production in s(NN)**(1/2) = 200-GeV Au + Au collisions."

description: The ratio of the hadronic decay photon $v_2$ over inclusive photon $v_2$ ($v_2^{b.g}/v_2^{inclusive \gamma}$) compared with the direct photon excess ratio $R = (N_{direct \gamma} + N_{b.g})/N_{b.g}$.
description: The azimuthal distribution of identified $\pi^0$ and inclusive photons has been measured in $\sqrt{s_{NN}}$ = 200 GeV Au+Au collisions with the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC). The second harmonic parameter ($v_2$) was measured to describe the observed anisotropy of the azimuthal distribution. The measured inclusive photon $v_2$ is consistent with the value expected for the photons from hadron decay and is also consistent with the lack of direct photon signal over the measured $p_T$ range 1 - 6 GeV/$c$. An attempt is made to extract $v_2$ of direct photons.
DOI: 10.17182/hepdata.142391.v1/t1
title: "Figure 2" of "Mid-rapidity direct-photon production in p+p collisions at s**(1/2) = 200-GeV"

description: Measured cross section and NLO pQCD calculations for direct-photon production in p+p collisions at $\sqrt{s}=$200 GeV. The normalization error of 9.6% is not shown. The two data points plotted with an arrow indicate the beginning of the low- and high-$p_\mathrm{T}$ ranges where the direct photon signal is consistent with zero. The upper edges of the arrows indicate an upper limit (90% confidence level) for the direct photon cross section calculated from the statistical and systematic uncertainty.
description: A measurement of direct photons in p+p collisions at $\sqrt{s}=200$~GeV is presented. A photon excess above background from $\pi^0 \rightarrow \gamma+\gamma$, $\eta\rightarrow \gamma+\gamma$ and other decays is observed in the transverse momentum range $5.5
DOI: 10.26093/cds/vizier.22720032
title: TKS. XX. Exoplanet masses & orbit parameters

description: VizieR online Data Catalogue associated with article published in journal Astrophysical Journal Supplement Series with title ' The TESS-Keck Survey. XX. 15 new TESS planets and a uniform RV analysis of all survey targets.' (bibcode: 2024ApJS..272...32P)
DOI: 10.17182/hepdata.142395.v1/t1
title: "Table 5" of "Measurements of $e^+e^-$ pairs from open heavy flavor in $p$+$p$ and $d$+$A$ collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Step by step extrapolation from the number of $e^+e^-$ pairs for $m_{e^+e^-}$ &gt; 1.16 GeV/$c^2$ from $c\bar{c}$ in the PHENIX acceptance to the number of $c\bar{c}$ pairs in 4$\pi$ for PYTHIA, MC@NLO, and POWHEG. Numbers are in units of pairs per event using the $c\bar{c}$ cross sections determined in this paper.
description: We report a measurement of $e^+e^−$ pairs from semileptonic heavy-flavor decays in $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $e^+e^−$ pair yield from $b\bar{b}$ and $c\bar{c}$ is separated by exploiting a double differential fit done simultaneously in dielectron invariant mass and $p_T$. We used three different event generators, PYTHIA, MC@ALO, and POWHEG, to simulate the $e^+e^−$ spectra from $c\bar{c}$ and $b\bar{b}$ production. The data can be well described by all three generators within the detector acceptance. However, when using the generators to extrapolate to 4$\pi$, significant differences are observed for the total cross section. These difference are less pronounced for $b\bar{b}$ than for $c\bar{c}$. The same model dependence was observed in already published $d$+$A$ data. The $p$+$p$ data are also directly compared with $d$+$A$ data in mass and $p_T$, and within the statistical accuracy no nuclear modification is seen.
DOI: 10.17182/hepdata.142395.v1/t2
title: "Table 6" of "Measurements of $e^+e^-$ pairs from open heavy flavor in $p$+$p$ and $d$+$A$ collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Step by step extrapolation from the number of $e^+e^-$ pairs for $m_{e^+e^-}$ &gt; 1.16 GeV/$c^2$ from $b\bar{b}$ in the PHENIX acceptance to the number of $b\bar{b}$ pairs in 4$\pi$ for PYTHIA, MC@NLO, and POWHEG. Numbers are in units of pairs per event using the $b\bar{b}$ cross sections determined in this paper.
description: We report a measurement of $e^+e^−$ pairs from semileptonic heavy-flavor decays in $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $e^+e^−$ pair yield from $b\bar{b}$ and $c\bar{c}$ is separated by exploiting a double differential fit done simultaneously in dielectron invariant mass and $p_T$. We used three different event generators, PYTHIA, MC@ALO, and POWHEG, to simulate the $e^+e^−$ spectra from $c\bar{c}$ and $b\bar{b}$ production. The data can be well described by all three generators within the detector acceptance. However, when using the generators to extrapolate to 4$\pi$, significant differences are observed for the total cross section. These difference are less pronounced for $b\bar{b}$ than for $c\bar{c}$. The same model dependence was observed in already published $d$+$A$ data. The $p$+$p$ data are also directly compared with $d$+$A$ data in mass and $p_T$, and within the statistical accuracy no nuclear modification is seen.
DOI: 10.17182/hepdata.142395.v1/t3
title: "Figure 13a" of "Measurements of $e^+e^-$ pairs from open heavy flavor in $p$+$p$ and $d$+$A$ collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Summary of $c\bar{c}$ and $b\bar{b}$ cross sections measured in $p$+$p$ collisions using three different generators, PYTHIA, MC@NLO, and POWHEG.
description: We report a measurement of $e^+e^−$ pairs from semileptonic heavy-flavor decays in $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $e^+e^−$ pair yield from $b\bar{b}$ and $c\bar{c}$ is separated by exploiting a double differential fit done simultaneously in dielectron invariant mass and $p_T$. We used three different event generators, PYTHIA, MC@ALO, and POWHEG, to simulate the $e^+e^−$ spectra from $c\bar{c}$ and $b\bar{b}$ production. The data can be well described by all three generators within the detector acceptance. However, when using the generators to extrapolate to 4$\pi$, significant differences are observed for the total cross section. These difference are less pronounced for $b\bar{b}$ than for $c\bar{c}$. The same model dependence was observed in already published $d$+$A$ data. The $p$+$p$ data are also directly compared with $d$+$A$ data in mass and $p_T$, and within the statistical accuracy no nuclear modification is seen.
DOI: 10.17182/hepdata.142395.v1/t4
title: "Figure 13b" of "Measurements of $e^+e^-$ pairs from open heavy flavor in $p$+$p$ and $d$+$A$ collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Summary of $c\bar{c}$ and $b\bar{b}$ cross sections measured in $d$+Au collisions expressed as nucleon-nucleon equivalent cross section by dividing the $d$+Au cross section by the average number of binary nucleon-nucleon collisions $N_{coll}$ = 7.6 $\pm$ 0.4.
description: We report a measurement of $e^+e^−$ pairs from semileptonic heavy-flavor decays in $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $e^+e^−$ pair yield from $b\bar{b}$ and $c\bar{c}$ is separated by exploiting a double differential fit done simultaneously in dielectron invariant mass and $p_T$. We used three different event generators, PYTHIA, MC@ALO, and POWHEG, to simulate the $e^+e^−$ spectra from $c\bar{c}$ and $b\bar{b}$ production. The data can be well described by all three generators within the detector acceptance. However, when using the generators to extrapolate to 4$\pi$, significant differences are observed for the total cross section. These difference are less pronounced for $b\bar{b}$ than for $c\bar{c}$. The same model dependence was observed in already published $d$+$A$ data. The $p$+$p$ data are also directly compared with $d$+$A$ data in mass and $p_T$, and within the statistical accuracy no nuclear modification is seen.
DOI: 10.17182/hepdata.142396.v1/t1
title: "Figure 6 (Spin-0)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HH\rightarrow \gamma\gamma bb$, as a function of X mass hypothesis. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 6 (upper) of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t2
title: "Figure 6 (Spin-2)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-2 resonance $X\rightarrow HH\rightarrow \gamma\gamma bb$, as a function of X mass hypothesis. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 6 (lower) of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t3
title: "Figure 7 (X mass = 300 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 300 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t4
title: "Figure 7 (X mass = 350 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 350 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t5
title: "Figure 7 (X mass = 400 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 400 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t6
title: "Figure 7 (X mass = 450 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 450 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t7
title: "Figure 7 (X mass = 500 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 500 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t8
title: "Figure 7 (X mass = 550 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 550 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t9
title: "Figure 7 (X mass = 600 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 600 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t10
title: "Figure 7 (X mass = 650 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 650 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t11
title: "Figure 7 (X mass = 700 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 700 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t12
title: "Figure 7 (X mass = 750 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 750 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t13
title: "Figure 7 (X mass = 800 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 800 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t14
title: "Figure 7 (X mass = 850 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 850 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t16
title: "Figure 7 (X mass = 950 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 950 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t15
title: "Figure 7 (X mass = 900 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 900 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142396.v1/t17
title: "Figure 7 (X mass = 1000 GeV)" of "Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% upper limits on the product of the production cross section and the branching fraction for a spin-0 resonance $X\rightarrow HY\rightarrow \gamma\gamma bb$, as a function of Y mass, for X mass = 1000 GeV. The $\pm1$ and $\pm2$ $\sigma$ uncertainty bands are given in addition to the expected median value. Numerical values provided in this table correspond to Figure 7 of the publication.
description: No data abstract available.
DOI: 10.17182/hepdata.142406.v1/t1
title: "Profile likelihood scan" of "Evidence for the Higgs boson decay to a $Z$ boson and a photon at the LHC"

description: The negative profile log-likelihood test statistic, where $\Lambda$ represents the likelihood ratio, as a function of the signal strength $\mu$ derived from the ATLAS data, the CMS data, and the combined result.
description: The first evidence for the Higgs boson decay to a $Z$ boson and a photon is presented, with a statistical significance of 3.4 standard deviations. The result is derived from a combined analysis of the searches performed by the ATLAS and CMS Collaborations with proton-proton collision data sets collected at the CERN Large Hadron Collider (LHC) from 2015 to 2018. These correspond to integrated luminosities of around 140 fb$^{-1}$ for each experiment, at a center-of-mass energy of 13 TeV. The measured signal yield is 2.2$\pm$0.7 times the Standard Model prediction, and agrees with the theoretical expectation within 1.9 standard deviations.
DOI: 10.17182/hepdata.142463.v1/t1
title: "pp_2TeV_multDist" of "Multiplicity dependence of charged-particle production in pp, p-Pb, Xe-Xe and Pb-Pb collisions at the LHC"

description: Charged-particle multiplicity distribution for pp collisions at 2.76 TeV.
description: CERN-LHC. ALICE. Multiplicity ($N_{\mathrm{ch}}$) distributions and transverse momentum ($p_{\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\eta| &lt; 0.8$ and $0.15\ \mathrm{GeV}/c &lt; p_{\mathrm{T}} &lt; 10\ \mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\sqrt{s_\mathrm{NN}} = 2.76\ \mathrm{TeV}$ up to $13\ \mathrm{TeV}$. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean and standard deviation derived from the multiplicity dependent $p_\mathrm{T}$ spectra are shown as a function of $N_{\mathrm{ch}}$. All observables are also extracted as a function of reltaive multiplicity $ N_{\mathrm{ch}}\ / &lt; N_{\mathrm{ch}} &gt; $.