cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.139988.v1/t3
title: "Table 3" of "Production of $b\bar{b}$ at forward rapidity in $p$+$p$ collisions at $\sqrt{s}=510$ GeV"

description: $b\bar{b}$ invariant yield measured via B meson decay to like-sign dimuons as a function of azimuthal opening angle. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC-PHENIX. The cross section of bottom quark-antiquark ($b\bar{b}$) production in $p$$+$$p$ collisions at $\sqrt{s_{NN}}$=510 GeV is measured with the PHENIX detector at the Relativistic Heavy Ion Collider. The results are based on the yield of high mass, like-sign muon pairs measured within the PHENIX muon arm acceptance $(1.2&lt;|y|&lt;2.2)$. The $b\bar{b}$ signal is extracted from like-sign dimuons by utilizing the unique properties of neutral $B$ meson oscillation. We report a differential cross section of $d\sigma_{b\bar{b}\rightarrow \mu^{\pm}\mu^{\pm}}/dy$=$0.16 \pm 0.01$ (stat)$\pm0.02$ (syst)$\pm0.02$ (global) nb for like-sign muons in the rapidity and $p_{T}$ ranges $1.2&lt;|y|&lt;2.2$ and $p_{T}&gt;1$ GeV/c, and dimuon mass of $5$-$10$ GeV/$c^{2}$. The extrapolated total cross section at this energy for $b\bar{b}$ production is $13.1 \pm 0.6 $(stat)$\pm 1.5$ (syst)$\pm 2.7$ (global) $\mu b$. The total cross section is compared to a perturbative quantum chromodynamics calculation and is consistent within uncertainties. The azimuthal opening angle between muon pairs from $b\bar{b}$ decays and their $p_{T}$ distributions are compared to distributions generated using PS PYTHIA6, which includes next-to-leading order processes. The azimuthal correlations and pair $p_{T}$ distribution are not very well described by PYTHIA calculations, but are still consistent within uncertainties. Flavor creation and flavor excitation subprocesses are favored over gluon splitting.
DOI: 10.17182/hepdata.139988.v1/t4
title: "Table 4" of "Production of $b\bar{b}$ at forward rapidity in $p$+$p$ collisions at $\sqrt{s}=510$ GeV"

description: $b\bar{b}$ invariant yield measured via B meson decay to like-sign dimuons as a function of pair $p_{T}$. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC-PHENIX. The cross section of bottom quark-antiquark ($b\bar{b}$) production in $p$$+$$p$ collisions at $\sqrt{s_{NN}}$=510 GeV is measured with the PHENIX detector at the Relativistic Heavy Ion Collider. The results are based on the yield of high mass, like-sign muon pairs measured within the PHENIX muon arm acceptance $(1.2&lt;|y|&lt;2.2)$. The $b\bar{b}$ signal is extracted from like-sign dimuons by utilizing the unique properties of neutral $B$ meson oscillation. We report a differential cross section of $d\sigma_{b\bar{b}\rightarrow \mu^{\pm}\mu^{\pm}}/dy$=$0.16 \pm 0.01$ (stat)$\pm0.02$ (syst)$\pm0.02$ (global) nb for like-sign muons in the rapidity and $p_{T}$ ranges $1.2&lt;|y|&lt;2.2$ and $p_{T}&gt;1$ GeV/c, and dimuon mass of $5$-$10$ GeV/$c^{2}$. The extrapolated total cross section at this energy for $b\bar{b}$ production is $13.1 \pm 0.6 $(stat)$\pm 1.5$ (syst)$\pm 2.7$ (global) $\mu b$. The total cross section is compared to a perturbative quantum chromodynamics calculation and is consistent within uncertainties. The azimuthal opening angle between muon pairs from $b\bar{b}$ decays and their $p_{T}$ distributions are compared to distributions generated using PS PYTHIA6, which includes next-to-leading order processes. The azimuthal correlations and pair $p_{T}$ distribution are not very well described by PYTHIA calculations, but are still consistent within uncertainties. Flavor creation and flavor excitation subprocesses are favored over gluon splitting.
DOI: 10.15468/dl.fk5qd6
title: Occurrence Download

description: A dataset containing 65 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Hippocampus camelopardalis",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 65 records from 8 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015996-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.5281/zenodo.17527158
title: Regards sur la Corruption : Entre Microéconomie et Économie Comportementale

description: Cet article explore les fondements de la corruption en croisant les approches microéconomiques et comportementales pour offrir une vision globale de ce phénomène complexe. Les théories économiques traditionnelles, telles que le modèle coûts-bénéfices de Becker (1968) et la théorie de l’agence, expliquent les comportements corruptifs par un calcul rationnel des bénéfices, des coûts et des probabilités de détection. Ces approches mettent l’accent sur la nécessité de renforcer la transparence institutionnelle, les mécanismes de contrôle et les sanctions pour limiter les opportunités de corruption. En parallèle, l’économie comportementale enrichit cette analyse en intégrant des dimensions psychologiques, notamment les biais cognitifs comme l’aversion aux pertes et l’effet de cadrage, ainsi que les émotions morales, telles que la culpabilité et la honte. Ces travaux montrent comment les normes sociales, la réciprocité et la confiance façonnent les dynamiques interpersonnelles au sein des réseaux corrompus. L’article souligne l’importance d’une approche intégrative qui combine les perspectives économiques et comportementales pour mieux comprendre et combattre la corruption.
DOI: 10.5281/zenodo.17527159
title: Regards sur la Corruption : Entre Microéconomie et Économie Comportementale

description: Cet article explore les fondements de la corruption en croisant les approches microéconomiques et comportementales pour offrir une vision globale de ce phénomène complexe. Les théories économiques traditionnelles, telles que le modèle coûts-bénéfices de Becker (1968) et la théorie de l’agence, expliquent les comportements corruptifs par un calcul rationnel des bénéfices, des coûts et des probabilités de détection. Ces approches mettent l’accent sur la nécessité de renforcer la transparence institutionnelle, les mécanismes de contrôle et les sanctions pour limiter les opportunités de corruption. En parallèle, l’économie comportementale enrichit cette analyse en intégrant des dimensions psychologiques, notamment les biais cognitifs comme l’aversion aux pertes et l’effet de cadrage, ainsi que les émotions morales, telles que la culpabilité et la honte. Ces travaux montrent comment les normes sociales, la réciprocité et la confiance façonnent les dynamiques interpersonnelles au sein des réseaux corrompus. L’article souligne l’importance d’une approche intégrative qui combine les perspectives économiques et comportementales pour mieux comprendre et combattre la corruption.
DOI: 10.17182/hepdata.140262.v1/t1
title: "Figure 1" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 1
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t2
title: "Figure 2ab" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 2ab
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t3
title: "Figure 2c" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 2c
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t4
title: "Figure 4a" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 4a
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t5
title: "Figure 4b" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 4b
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t6
title: "Figure 4c" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 4c
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t7
title: "Figure 5a" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 5a
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t10
title: "Figure 7" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 7
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t11
title: "Figure 8a" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 8a
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t12
title: "Figure 8b" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 8b
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t13
title: "Figure 8c" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 8c
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t14
title: "Figure 9a" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 9a
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t15
title: "Figure 9b" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 9b
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t16
title: "Figure 9c" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 9c
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t8
title: "Figure 5b" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 5b
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t9
title: "Figure 5c" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 5c
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t18
title: "Figure 10b" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 10b
description: No data abstract available.
DOI: 10.17182/hepdata.140262.v1/t19
title: "Figure 10c" of "Event-by-event correlations between $\Lambda$ ($\bar{\Lambda}$) hyperon global polarization and handedness with charged hadron azimuthal separation in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 27 \text{ GeV}$ from STAR"

description: Figure 10c
description: No data abstract available.
DOI: 10.17182/hepdata.140263.v1/t1
title: "Figure 1" of "Improved measurement of double helicity asymmetry in inclusive midrapidity pi0 production for polarized p + p collisions at s**(1/2) = 200-GeV."

description: Run-3+Run-4 combined results on $A^{\pi^0}_{LL}$ versus mean $p_T$ in each bin. Not included in the figure/table: the correlated for all points scale systematic uncertainty of 18% (scales both the values and stat. uncertainties by the same factor).
description: We present an improved measurement of the double helicity asymmetry for $\pi^0$ production in polarized proton-proton scattering at $\sqrt{s}$ = 200 GeV employing the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). The improvements to our previous measurement come from two main factors: Inclusion of a new data set from the 2004 RHIC run with higher beam polarizations than the earlier run and a recalibration of the beam polarization measurements, which resulted in reduced uncertainties and increased beam polarizations. The results are compared to a Next to Leading Order (NLO) perturbative Quantum Chromodynamics (pQCD) calculation with a range of polarized gluon distributions.
DOI: 10.17182/hepdata.140309.v1/t1
title: "Table 1" of "Collision-energy Dependence of Deuteron Cumulants and Proton-deuteron Correlations in Au+Au collisions at RHIC"

description: Cumulants of the deuteron number distributions as a function of collision energy (from $\sqrt{s_{NN}}$ = 7.7 - 200 GeV) for most central (0 - 5$\%$), mid-central (30 - 40$\%$), and peripheral (70 - 80$\%$) Au+Au collisions. Cumulants are corrected for detector efficiency and centrality bin-width effect.
description: No data abstract available.
DOI: 10.17182/hepdata.140309.v1/t2
title: "Table 2" of "Collision-energy Dependence of Deuteron Cumulants and Proton-deuteron Correlations in Au+Au collisions at RHIC"

description: Cumulant ratios C2/C1, C3/C2, C4/C2 of deuteron number distributions and the Pearson correlation co-efficient between deuteron and proton distributions in 0-5$\%$ and 70-80$\%$ centralities in Au+Au collisions at nine energies from $\sqrt{s_{NN}}$ = 7.7 - 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140309.v1/t3
title: "Table 3" of "Collision-energy Dependence of Deuteron Cumulants and Proton-deuteron Correlations in Au+Au collisions at RHIC"

description: Cumulant ratio C4/C2 of deuteron number distributions in 0-5$\%$ centrality in Au+Au collisions at nine energies from $\sqrt{s_{NN}}$ = 7.7 - 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140310.v1/t1
title: "Table 1" of "Search for dark photons in rare $Z$ boson decays with the ATLAS detector"

description: Observed and expected upper limits at 95% CL on the production cross-section times branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 20 GeV
description: A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using $139~fb^{-1}$ of $\sqrt{s} = 13$ TeV proton--proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\epsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.
DOI: 10.17182/hepdata.140310.v1/t2
title: "Table 2" of "Search for dark photons in rare $Z$ boson decays with the ATLAS detector"

description: Observed and expected upper limits at 95% CL on the production cross-section times branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 30 GeV
description: A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using $139~fb^{-1}$ of $\sqrt{s} = 13$ TeV proton--proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\epsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.
DOI: 10.17182/hepdata.140310.v1/t3
title: "Table 3" of "Search for dark photons in rare $Z$ boson decays with the ATLAS detector"

description: Observed and expected upper limits at 95% CL on the production cross-section times branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 40 GeV
description: A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using $139~fb^{-1}$ of $\sqrt{s} = 13$ TeV proton--proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\epsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.
DOI: 10.17182/hepdata.140310.v1/t10
title: "Table 10" of "Search for dark photons in rare $Z$ boson decays with the ATLAS detector"

description: Observed 90% CL upper limits on $\alpha_{D}\epsilon^{2}$ as a function of $m_{A'}$ at dark Higgs boson mass of 50 GeV
description: A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using $139~fb^{-1}$ of $\sqrt{s} = 13$ TeV proton--proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\epsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.
DOI: 10.17182/hepdata.140310.v1/t11
title: "Table 11" of "Search for dark photons in rare $Z$ boson decays with the ATLAS detector"

description: Observed 90% CL upper limits on $\alpha_{D}\epsilon^{2}$ as a function of $m_{A'}$ at dark Higgs boson mass of 60 GeV
description: A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using $139~fb^{-1}$ of $\sqrt{s} = 13$ TeV proton--proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\epsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.
DOI: 10.17182/hepdata.140310.v1/t4
title: "Table 4" of "Search for dark photons in rare $Z$ boson decays with the ATLAS detector"

description: Observed and expected upper limits at 95% CL on the production cross-section times branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 50 GeV
description: A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using $139~fb^{-1}$ of $\sqrt{s} = 13$ TeV proton--proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\epsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.