cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.qs989s
title: Occurrence Download

description: A dataset containing 1156 species occurrences available in GBIF matching the query:
{
 "and" : [
 "GadmGid is one of (CHN.31.1_1, CHN.31.3_1, CHN.31.2_1, CHN.31.8_1, CHN.31.6_1)",
 "TaxonKey is Bambusicola thoracicus (Temminck, 1815)"
 ]
}

 The dataset includes 1156 records from 4 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048022-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.34740/kaggle/dsv/9107992
title: canny_images
DOI: 10.15468/dl.ef6ug5
title: Occurrence Download

description: A dataset containing 2 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-10.22481 35.40386,15.22481 35.40386,15.22481 45.59614,-10.22481 45.59614,-10.22481 35.40386))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Paragus quadrifasciatus Say, 1824"
 ]
}

 The dataset includes 2 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048024-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.4578xh
title: Occurrence Download

description: A dataset containing 0 species occurrences available in GBIF matching the query:
{
 "Geometry" : [
 "POLYGON ((147.15677 -35.834501, 147.15677 -35.838992, 147.163508 -35.838992, 147.163508 -35.834501, 147.15677 -35.834501))"
 ]
}

 The dataset includes 0 records from 0 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048028-240626123714530/datasets/export for details.
DOI: 10.15468/dl.3wyj2b
title: Occurrence Download

description: A dataset containing 5563 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((46.90678 3.12994,181.09322 3.12994,181.09322 56.87006,46.90678 56.87006,46.90678 3.12994))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Propylea japonica (Thunberg, 1781)"
 ]
}

 The dataset includes 5563 records from 56 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048026-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.p4359v
title: Occurrence Download

description: A dataset containing 17675 species occurrences available in GBIF matching the query:
{
 "and" : [
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "TaxonKey is Centrocercus urophasianus (Bonaparte, 1827)"
 ]
}

 The dataset includes 17675 records from 58 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048029-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.awqcyt
title: Occurrence Download

description: A dataset containing 825 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((67.15938 15.94234,154.84062 15.94234,154.84062 51.05766,67.15938 51.05766,67.15938 15.94234))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Lysiphlebia japonica (Ashmead, 1906)"
 ]
}

 The dataset includes 825 records from 3 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048030-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.w9t7yw
title: Occurrence Download

description: A dataset containing 118 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Bombus keriensis Morawitz, 1887"
 ]
}

 The dataset includes 118 records from 11 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048031-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.6kczu3
title: Occurrence Download

description: A dataset containing 0 species occurrences available in GBIF matching the query:
{
 "Geometry" : [
 "MULTIPOLYGON (((147.271306 -35.838992, 147.271306 -35.841238, 147.273552 -35.841238, 147.273552 -35.838992, 147.271306 -35.838992)), ((147.273552 -35.841238, 147.273552 -35.843484, 147.278043 -35.843484, 147.278043 -35.841238, 147.273552 -35.841238)))"
 ]
}

 The dataset includes 0 records from 0 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048032-240626123714530/datasets/export for details.
DOI: 10.15468/dl.ut8xkf
title: Occurrence Download

description: A dataset containing 157 species occurrences available in GBIF matching the query:
{
 "and" : [
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Chrysopa septempunctata Wesmael, 1841"
 ]
}

 The dataset includes 157 records from 14 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048033-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.zpsurc
title: Occurrence Download

description: A dataset listing the 1 species recorded in GBIF matching the query:
{
 "and" : [
 "BasisOfRecord is one of (Human Observation, Machine Observation)",
 "DatasetKey is one of (Welsh Invertebrate Database (WID), Observation.org, Nature data from around the World, Threatened species occurrences, Denmark 1991-2015, NRW Regional Data: South East Wales Non-sensitive species, Artportalen, Dutch Foundation for Applied Water Research (STOWA) - Limnodata Neerlandica, Inventaire national des araignées de France métropolitaine, Plan d'actions du Canal des Deux mers en Midi Pyrénées-Données patrimoine naturel Canal des deux mers et Canal du Midi, naturgucker, iRecord Surveys)",
 "OccurrenceStatus is Present",
 "TaxonKey is Dolomedes plantarius (Clerck, 1757)",
 "Year 2004-2013"
 ]
}

 The dataset's 1 records were derived from 10 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048009-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.tvb5xf
title: Occurrence Download

description: A dataset listing the 62394 species recorded in GBIF matching the query:
{
 "and" : [
 "Continent is Asia",
 "Country is China",
 "Year 1970-2000"
 ]
}

 The dataset's 62394 records were derived from 1418 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0048006-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.153410.v1/t2
title: "$\gamma p \to \omega\pi^0\pi^0p$ Cross Sections" of "An Upper Limit on the Photoproduction Cross Section of the Spin-Exotic $\pi_1(1600)$"

description: Measured $\sigma(\gamma p\to\omega\pi^0\pi^0p)$ values for $8
description: No data abstract available.
DOI: 10.17182/hepdata.158374.v1/t1
title: "Figure 4" of "Measurement of inclusive jet cross section and substructure in $p$+$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: The jet differential cross section as a function of jet $p_T$. Statistical uncertainties are typically smaller than the data points while systematic uncertainties are shown with boxes. An overall normalization systematic of 7% is not included in the point-by-point systematic uncertainties.
description: The jet cross section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0
DOI: 10.17182/hepdata.158374.v1/t3
title: "Figure 6 Part 1" of "Measurement of inclusive jet cross section and substructure in $p$+$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: $\xi$ distributions for different jet $p_T$ bins.
description: The jet cross section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0
DOI: 10.17182/hepdata.158374.v1/t4
title: "Figure 6 Part 2" of "Measurement of inclusive jet cross section and substructure in $p$+$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: $\xi$ distributions for different jet $p_T$ bins.
description: The jet cross section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0
DOI: 10.17182/hepdata.158374.v1/t5
title: "Figure 6 Part 3" of "Measurement of inclusive jet cross section and substructure in $p$+$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: $\xi$ distributions for different jet $p_T$ bins.
description: The jet cross section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0
DOI: 10.17182/hepdata.158374.v1/t7
title: "Figure 7 Part 2" of "Measurement of inclusive jet cross section and substructure in $p$+$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: The $j_T/p_{T}^{\rm jet}$ distributions for different jet $p_T$ bins.
description: The jet cross section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0
DOI: 10.17182/hepdata.158374.v1/t8
title: "Figure 8" of "Measurement of inclusive jet cross section and substructure in $p$+$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: $r$ distributions for different jet $p_T$ bins.
description: The jet cross section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0
DOI: 10.17182/hepdata.158374.v1/t6
title: "Figure 7 Part 1" of "Measurement of inclusive jet cross section and substructure in $p$+$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: The $j_T/p_{T}^{\rm jet}$ distributions for different jet $p_T$ bins.
description: The jet cross section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0
DOI: 10.17182/hepdata.167351.v1/t1
title: "Table 1" of "The Asymmetry of Antimatter in the Proton"

description: Cross section ratios $\sigma_{D}/2\sigma_{H}$ binned in $x_t$ with their statistical and systematic uncertainties and the average values for the kinematic variables of each $x_t$ bin. The cross section ratios are defined as the ratio of luminosity-corrected yields from the hydrogen and deuterium targets. The final column is the experimental resolution in $x_t$ as determined by Monte Carlo simulations.
description: No data abstract available.
DOI: 10.17182/hepdata.167351.v1/t2
title: "Table 2" of "The Asymmetry of Antimatter in the Proton"

description: Ratios of $\bar{d}(x)$ to $\bar{u}(x)$ with their upper and lower statistical and systematic uncertainties. The analysis was based on the present cross section ratio data, and next-to-leading order calculations of the Drell-Yan cross sections using CT18 parton distributions for all except the ratio of $\bar{d}(x)$ to $\bar{u}(x)$. The systematic uncertainty is fully correlated among all $x$ bins. The systematic uncertainty does not include a contribution from the choice of the base (CT18) pdf, which is small if added in quadrature to the other systematic uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.167351.v1/t3
title: "Extended Data Table 1" of "The Asymmetry of Antimatter in the Proton"

description: Ratios of $\mathbf{\sigma_D}$ to $\mathbf{2\sigma_H}$ as a function of $\mathbf{P_T}$. Ratios of $\sigma_D$ to $2\sigma_H$ with their statistical and systematic uncertainties as a function of transverse momentum, $P_T$. The cross section ratios are defined as the ratio of luminosity-corrected yields from the hydrogen and deuterium targets. The final column, $\delta P_T$ is the experimental resolution in $P_T$ as determined by Monte Carlo simulation.
description: No data abstract available.
DOI: 10.17182/hepdata.167351.v1/t4
title: "Extended Data Table 2" of "The Asymmetry of Antimatter in the Proton"

description: Ratios of $\mathbf{\sigma_D}$ to $\mathbf{2\sigma_H}$ as a function of $\mathbf{M}$. Ratios of $\sigma_D$ to $2\sigma_H$ with their statistical and systematic uncertainties as a function of mass, $M$. The cross section ratios are defined as the ratio of luminosity-corrected yields from the hydrogen and deuterium targets. The final column, $\delta M$ is the experimental resolution in $M$ as determined by Monte Carlo simulation.
description: No data abstract available.
DOI: 10.17182/hepdata.167351.v1/t5
title: "Extended Data Table 3" of "The Asymmetry of Antimatter in the Proton"

description: The acceptance relative to a $4\pi$ detector and average kinematic values for bins in $x_t$ and $x_b$.
description: No data abstract available.
DOI: 10.57783/3vze-a598
title: LibreChat
DOI: 10.17182/hepdata.131759.v1/t1
title: "Figure 1" of "Transverse single spin asymmetries of forward neutrons in $p+p$, $p+$Al and $p+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV as a function of transverse and longitudinal momenta"

description: Measured forward neutron single spin asymmetries in p+p collisions as a function of pT in bins of xF
description: BNL-RHIC. In 2015, the PHENIX collaboration has taken p+p, p+Al and p+Au collision data at center of mass energies of $\sqrt{s_{NN}}=200$ GeV with the proton beam(s) transversely polarized. At very forward rapidities $\eta&gt;6.8$ relative to the polarized proton beam, neutrons were detected either inclusively or in (anti)correlation with detector activity related to hard collisions. The resulting single spin asymmetries, that were already previously reported, have now been extracted as a function of the transverse momentum of the neutron as well as its longitudinal momentum fraction $x_F$. The explicit kinematic dependence, combined with the correlation information allows for a closer look at the interplay of different mechanisms suggested to describe these asymmetries, such as hadronic interactions or electromagnetic interactions in ultra-peripheral collisions, UPC.
DOI: 10.17182/hepdata.131759.v1/t2
title: "Figure 2" of "Transverse single spin asymmetries of forward neutrons in $p+p$, $p+$Al and $p+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV as a function of transverse and longitudinal momenta"

description: Measured forward neutron single spin asymmetries in p+Al collisions as a function of pT in bins of xF
description: BNL-RHIC. In 2015, the PHENIX collaboration has taken p+p, p+Al and p+Au collision data at center of mass energies of $\sqrt{s_{NN}}=200$ GeV with the proton beam(s) transversely polarized. At very forward rapidities $\eta&gt;6.8$ relative to the polarized proton beam, neutrons were detected either inclusively or in (anti)correlation with detector activity related to hard collisions. The resulting single spin asymmetries, that were already previously reported, have now been extracted as a function of the transverse momentum of the neutron as well as its longitudinal momentum fraction $x_F$. The explicit kinematic dependence, combined with the correlation information allows for a closer look at the interplay of different mechanisms suggested to describe these asymmetries, such as hadronic interactions or electromagnetic interactions in ultra-peripheral collisions, UPC.
DOI: 10.17182/hepdata.132920.v1/t1
title: "SDME results" of "Measurement of Spin Density Matrix Elements in $\Lambda(1520)$ Photoproduction at 8.2-8.8 GeV"

description: Numerical results for all presented SDMEs. The first uncertainty is statistical, the second systematic
description: "Results and supplementary material for Measurement of spin density matrix elements in Λ(1520) photoproduction at 8.2-8.8 GeV"
DOI: 10.17182/hepdata.132920.v1/t2
title: "Naturality results" of "Measurement of Spin Density Matrix Elements in $\Lambda(1520)$ Photoproduction at 8.2-8.8 GeV"

description: Numerical results for all presented natural and unnatural combinations, and covariances between $\rho^1_{11}$ and $\rho^1_{33}$. The first uncertainty is statistical, the second systematic
description: "Results and supplementary material for Measurement of spin density matrix elements in Λ(1520) photoproduction at 8.2-8.8 GeV"
DOI: 10.17182/hepdata.132920.v1/t3
title: "Markov Chain Bin 1" of "Measurement of Spin Density Matrix Elements in $\Lambda(1520)$ Photoproduction at 8.2-8.8 GeV"

description: This table contains thinned out samples of the Markov chains used in the parameter estimation of the SDME measurements for $-(t-t_\text{0}) = 0.197\pm0.069~\text{GeV}^2/c^2$, reported in the main article. One in about 250 steps in the chain, which results in 200 different sets of SDMEs, is provided. These values should be used instead of bootstrapping of the results, in order to estimate uncertainties of physics models fitted to this data. To assess how the uncertainties propagate to the model uncertainties, one should evaluate the model under scrutiny for each of the 200 different sets of SDMEs. Plotting all resulting lines in a single plot will create bands which reflect the influence of the uncertainties in the data on the model. This method has the great advantage that all correlations are accurately taken into account.
description: "Results and supplementary material for Measurement of spin density matrix elements in Λ(1520) photoproduction at 8.2-8.8 GeV"
DOI: 10.17182/hepdata.132920.v1/t4
title: "Markov Chain Bin 2" of "Measurement of Spin Density Matrix Elements in $\Lambda(1520)$ Photoproduction at 8.2-8.8 GeV"

description: This table contains thinned out samples of the Markov chains used in the parameter estimation of the SDME measurements for $-(t-t_\text{0}) = 0.400\pm0.056~\text{GeV}^2/c^2$, reported in the main article. One in about 250 steps in the chain, which results in 200 different sets of SDMEs, is provided. These values should be used instead of bootstrapping of the results, in order to estimate uncertainties of physics models fitted to this data. To assess how the uncertainties propagate to the model uncertainties, one should evaluate the model under scrutiny for each of the 200 different sets of SDMEs. Plotting all resulting lines in a single plot will create bands which reflect the influence of the uncertainties in the data on the model. This method has the great advantage that all correlations are accurately taken into account.
description: "Results and supplementary material for Measurement of spin density matrix elements in Λ(1520) photoproduction at 8.2-8.8 GeV"
DOI: 10.17182/hepdata.132920.v1/t5
title: "Markov Chain Bin 3" of "Measurement of Spin Density Matrix Elements in $\Lambda(1520)$ Photoproduction at 8.2-8.8 GeV"

description: This table contains thinned out samples of the Markov chains used in the parameter estimation of the SDME measurements for $-(t-t_\text{0}) = 0.597\pm0.057~\text{GeV}^2/c^2$, reported in the main article. One in about 250 steps in the chain, which results in 200 different sets of SDMEs, is provided. These values should be used instead of bootstrapping of the results, in order to estimate uncertainties of physics models fitted to this data. To assess how the uncertainties propagate to the model uncertainties, one should evaluate the model under scrutiny for each of the 200 different sets of SDMEs. Plotting all resulting lines in a single plot will create bands which reflect the influence of the uncertainties in the data on the model. This method has the great advantage that all correlations are accurately taken into account.
description: "Results and supplementary material for Measurement of spin density matrix elements in Λ(1520) photoproduction at 8.2-8.8 GeV"
DOI: 10.17182/hepdata.131759.v1/t3
title: "Figure 3" of "Transverse single spin asymmetries of forward neutrons in $p+p$, $p+$Al and $p+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV as a function of transverse and longitudinal momenta"

description: Measured forward neutron single spin asymmetries in p+Au collisions as a function of pT in bins of xF
description: BNL-RHIC. In 2015, the PHENIX collaboration has taken p+p, p+Al and p+Au collision data at center of mass energies of $\sqrt{s_{NN}}=200$ GeV with the proton beam(s) transversely polarized. At very forward rapidities $\eta&gt;6.8$ relative to the polarized proton beam, neutrons were detected either inclusively or in (anti)correlation with detector activity related to hard collisions. The resulting single spin asymmetries, that were already previously reported, have now been extracted as a function of the transverse momentum of the neutron as well as its longitudinal momentum fraction $x_F$. The explicit kinematic dependence, combined with the correlation information allows for a closer look at the interplay of different mechanisms suggested to describe these asymmetries, such as hadronic interactions or electromagnetic interactions in ultra-peripheral collisions, UPC.
DOI: 10.17182/hepdata.131759.v1/t4
title: "Figure 4" of "Transverse single spin asymmetries of forward neutrons in $p+p$, $p+$Al and $p+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV as a function of transverse and longitudinal momenta"

description: Forward neutron single spin asymmetries in p+p, p+Al and p+Au collisions as a function of pT in bins of xF correlated with hard collision activity
description: BNL-RHIC. In 2015, the PHENIX collaboration has taken p+p, p+Al and p+Au collision data at center of mass energies of $\sqrt{s_{NN}}=200$ GeV with the proton beam(s) transversely polarized. At very forward rapidities $\eta&gt;6.8$ relative to the polarized proton beam, neutrons were detected either inclusively or in (anti)correlation with detector activity related to hard collisions. The resulting single spin asymmetries, that were already previously reported, have now been extracted as a function of the transverse momentum of the neutron as well as its longitudinal momentum fraction $x_F$. The explicit kinematic dependence, combined with the correlation information allows for a closer look at the interplay of different mechanisms suggested to describe these asymmetries, such as hadronic interactions or electromagnetic interactions in ultra-peripheral collisions, UPC.