cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141648.v1/t6
title: "Figure 6" of "Centrality dependence of the high p(T) charged hadron suppression in Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: The top panel gives the nuclear modification factor $R_{AA}$ for three exclusive $p_T$ regions as a function of the centrality of the collision. The lower panel shows essentially the same quantity but normalized to the number of participant pairs rather than to the number of binary collisions. The dotted line indicates the expectation for scaling with the number of binary collisions (top) or with the number of participants (bottom). Only statistical errors are shown. The systematic error on the scale and the centrality dependence are identical to the errors shown in Fig. 5. These errors are correlated, i.e. take their maximum or minimum value simultaneously for all centrality and $p_T$ selections. In addition, there are also $p_T$ dependent systematic errors, which are given in Table 1. The systematic errors do not alter the trends in the data.
description: PHENIX has measured the centrality dependence of charged hadron $p_T$ spectra from Au + Au collisions at $\sqrt{s_{NN}}$ = 130 GeV. The truncated mean $p_T$ decreases with centrality for $p_T$ $&gt;$ 2 GeV/$c$, indicating an apparent reduction of the contribution from hard scattering to high $p_T$ hadron production. For central collisions the yield at high $p_T$ is shown to be suppressed compared to binary nucleon-nucleon collision scaling of p+p data. This suppression is monotonically increasing with centrality, but most of the change occurs below 30% centrality, i.e. for collisions with less than $~$ 140 participating nucleons. The observed $p_T$ and centrality dependence is consistent with the particle production predicted by models including hard scattering and subsequent energy loss of the scattered partons in the dense matter created in the collisions.
DOI: 10.17182/hepdata.141649.v1/t1
title: "Figure 1a-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t2
title: "Figure 1a-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t3
title: "Figure 1b-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t4
title: "Figure 1b-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t5
title: "Figure 1c-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t6
title: "Figure 1c-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.6084/m9.figshare.28029611.v10
title: Data Dictionary for CLEAR Relational Database.zip

description: Data Dictionary (Codebook) for CLEAR Relational Database
DOI: 10.17182/hepdata.141649.v1/t10
title: "Figure 2b-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t7
title: "Figure 2a-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t8
title: "Figure 2a-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t9
title: "Figure 2b-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.15468/dl.m6eyaq
title: Occurrence Download

description: A dataset containing 788 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-81.94719 33.44101,-81.94719 33.51164,-82.04864 33.51164,-82.04864 33.44101,-81.94719 33.44101))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Magnoliopsida",
 "Year 2000-2025"
 ]
}

 The dataset includes 788 records from 8 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015999-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.141649.v1/t11
title: "Figure 2c-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t12
title: "Figure 2c-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t13
title: "Figure 2d-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t14
title: "Figure 2d-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t15
title: "Figure 3a-1" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $k_T$ dependence of extracted spheroidal source parameters for pion source functions (a) $R_T$ , (b) $a$, and (c) $\lambda$ for most central collisions & perhipheral collisions.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t16
title: "Figure 3a-2" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $k_T$ dependence of extracted spheroidal source parameters for pion source functions (a) $R_T$ , (b) $a$, and (c) $\lambda$ for most central collisions & perhipheral collisions.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141649.v1/t17
title: "Figure 3b" of "Evidence for a long-range component in the pion emission source in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $k_T$ dependence of extracted spheroidal source parameters for pion source functions (a) $R_T$ , (b) $a$, and (c) $\lambda$ for most central collisions & perhipheral collisions.
description: Emission source functions are extracted from correlation functions constructed from charged pions produced at mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The source parameters extracted from these functions at low $k_T$, give first indications of a long tail for the pion emission source. The source extension cannot be explained solely by simple kinematic considerations. The possible role of a halo of secondary pions from resonance emissions is explored.
DOI: 10.17182/hepdata.141650.v1/t1
title: "Table 1" of "Measurement and interpretation of same-sign $W$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Fiducial differential cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\ell\ell}$.
The correlation of uncertainties of the measured cross section across bins is presented in Table 11.
description: This paper presents the measurement of fiducial and differential cross sections for both the inclusive and electroweak production of a same-sign $W$-boson pair in association with two jets ($W^\pm W^\pm jj$) using $139\,\mathrm{fb}^{-1}$ of proton--proton collision data recorded at a centre-of-mass energy of $\sqrt{s}=13$ TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity difference. The measured fiducial cross sections for electroweak and inclusive $W^\pm W^\pm jj$ production are $2.92 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb and $3.38 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95\%\ confidence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons \(H^{\pm\pm}\) that are produced in vector-boson fusion processes and decay into a same-sign $W$ boson pair is performed. The largest deviation from the Standard Model occurs for an \(H^{\pm\pm}\) mass near $450\,\mathrm{GeV}$, with a global significance of 2.5 standard deviations.
DOI: 10.17182/hepdata.141650.v1/t2
title: "Table 2" of "Measurement and interpretation of same-sign $W$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Fiducial differential cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{T}}$.
The correlation of uncertainties of the measured cross section across bins is presented in Table 12.
description: This paper presents the measurement of fiducial and differential cross sections for both the inclusive and electroweak production of a same-sign $W$-boson pair in association with two jets ($W^\pm W^\pm jj$) using $139\,\mathrm{fb}^{-1}$ of proton--proton collision data recorded at a centre-of-mass energy of $\sqrt{s}=13$ TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity difference. The measured fiducial cross sections for electroweak and inclusive $W^\pm W^\pm jj$ production are $2.92 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb and $3.38 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95\%\ confidence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons \(H^{\pm\pm}\) that are produced in vector-boson fusion processes and decay into a same-sign $W$ boson pair is performed. The largest deviation from the Standard Model occurs for an \(H^{\pm\pm}\) mass near $450\,\mathrm{GeV}$, with a global significance of 2.5 standard deviations.
DOI: 10.17182/hepdata.141650.v1/t10
title: "Table 10" of "Measurement and interpretation of same-sign $W$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$.
The correlation of uncertainties of the measured cross section across bins is presented in Table 20.
description: This paper presents the measurement of fiducial and differential cross sections for both the inclusive and electroweak production of a same-sign $W$-boson pair in association with two jets ($W^\pm W^\pm jj$) using $139\,\mathrm{fb}^{-1}$ of proton--proton collision data recorded at a centre-of-mass energy of $\sqrt{s}=13$ TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity difference. The measured fiducial cross sections for electroweak and inclusive $W^\pm W^\pm jj$ production are $2.92 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb and $3.38 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95\%\ confidence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons \(H^{\pm\pm}\) that are produced in vector-boson fusion processes and decay into a same-sign $W$ boson pair is performed. The largest deviation from the Standard Model occurs for an \(H^{\pm\pm}\) mass near $450\,\mathrm{GeV}$, with a global significance of 2.5 standard deviations.
DOI: 10.17182/hepdata.141650.v1/t3
title: "Table 3" of "Measurement and interpretation of same-sign $W$ boson pair production in association with two jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Fiducial differential cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{jj}}$.
The correlation of uncertainties of the measured cross section across bins is presented in Table 13.
description: This paper presents the measurement of fiducial and differential cross sections for both the inclusive and electroweak production of a same-sign $W$-boson pair in association with two jets ($W^\pm W^\pm jj$) using $139\,\mathrm{fb}^{-1}$ of proton--proton collision data recorded at a centre-of-mass energy of $\sqrt{s}=13$ TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity difference. The measured fiducial cross sections for electroweak and inclusive $W^\pm W^\pm jj$ production are $2.92 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb and $3.38 \pm 0.22\, \text{(stat.)} \pm 0.19\, \text{(syst.)}$ fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95\%\ confidence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons \(H^{\pm\pm}\) that are produced in vector-boson fusion processes and decay into a same-sign $W$ boson pair is performed. The largest deviation from the Standard Model occurs for an \(H^{\pm\pm}\) mass near $450\,\mathrm{GeV}$, with a global significance of 2.5 standard deviations.