cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.116554.v1/t2
title: "Table 1-2" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 200 GeV measurements of the two and four-particle elliptic flow and the elliptic flow fluctuations of the K particle.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.17182/hepdata.116554.v1/t4
title: "Table 2-1" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 200 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.17182/hepdata.116553.v1/t15
title: "Figure 12 Bottom panel" of "Di-electron spectrum at mid-rapidity in $p+p$ collisions at $\sqrt{s} = 200$ GeV"

description: Data over cocktail ratio after efficiency correction within the STAR acceptance in $\sqrt{s}$ = 200GeV NSD p + p collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.116553.v1/t16
title: "Figure 15" of "Di-electron spectrum at mid-rapidity in $p+p$ collisions at $\sqrt{s} = 200$ GeV"

description: The ω → $e^+ e^-$ invariant yield, divided by its B.R. in $\sqrt{s}$ = 200GeV NSD p + p collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.116554.v1/t3
title: "Table 1-3" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 200 GeV measurements of the two and four-particle elliptic flow and the elliptic flow fluctuations of the p particle.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.17182/hepdata.116554.v1/t5
title: "Table 2-2" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 54.4 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.17182/hepdata.116554.v1/t11
title: "Table 3-2" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Cu+Au 200 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.17182/hepdata.116554.v1/t6
title: "Table 2-3" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 39 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.25549/vercoutere-ouc110611929
title: Woven wall hanging with multi-colored lengthwise stripes

description: Purple, yellow, orange, and pink vertical (warp) thin thread lines with brownish gray yarn background (weft),
DOI: 10.17182/hepdata.116554.v1/t10
title: "Table 3-1" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The U+U 193 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.17182/hepdata.116554.v1/t8
title: "Table 2-5" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 19.6 GeV measurements of the two- and four-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.15468/dl.k93y7e
title: Occurrence Download

description: A dataset containing 85442454 species occurrences available in GBIF matching the query:
{
 "and" : [
 "BasisOfRecord is Human Observation",
 "CoordinateUncertaintyInMeters 0.0-1000.0",
 "Geometry POLYGON((-125.63503 34.57157,-120.78511 33.04002,-118.61542 31.38084,-97.42897 25.25464,-75.34911 24.36122,-65.39403 47.71738,-125.25214 49.75945,-125.63503 34.57157))"
 ]
}

 The dataset includes 85442454 records from 573 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015940-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.116554.v1/t7
title: "Table 2-4" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 27 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.17182/hepdata.116554.v1/t9
title: "Table 2-6" of "Collision-system and beam-energy dependence of anisotropic flow fluctuations"

description: The Au+Au 11.5 GeV measurements of the two- and four-particle elliptic flow and the elliptic flow fluctuations.
description: "Collision-system and beam-energy dependence of anisotropic flow fluctuations."
DOI: 10.25549/vercoutere-ouc110611933
title: Woven wall hanging in white and black

description: Black warp thread and white weft yarn creating a center diamond design flanked by a zig zag design on each side. Gold metallic thread interwoven with black thread. Black border on each vertical end next to the fringe.
DOI: 10.15468/dl.kwt28y
title: Occurrence Download

description: A dataset containing 3083 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Acacia mangium"
 ]
}

 The dataset includes 3083 records from 265 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015948-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.25549/vercoutere-ouc110637164
title: Rustic clay vase similar to a Greek amphora

description: Brown clay vase painted with black, brown, green and yellow geometric shapes; exterior has bumpy surface; made with a potter's wheel; two handle stubs attached to the shoulder
DOI: 10.25549/vercoutere-ouc110637189
title: Woman's head sculpture with ash tray molded in clay

description: White glazed molded clay sculpture of a woman with shoulder length hair; includes a small receptacle for ashes or other at the ottom front
DOI: 10.17182/hepdata.126972.v1/t1
title: "Table_T01" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.996
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.25549/vercoutere-ouc110637192
title: Woman's head sculpture with ash tray molded in clay

description: White glazed molded clay sculpture of a woman with shoulder length hair; includes a small receptacle for ashes or other at the ottom front
DOI: 10.17182/hepdata.126972.v1/t2
title: "Table_T02" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.966
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t3
title: "Table_T03" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.906
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t4
title: "Table_T04" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.819
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t5
title: "Table_T05" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.707
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t6
title: "Table_T06" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.574
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t7
title: "Table_T07" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.423
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t10
title: "Table_T10" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.087
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t12
title: "Table_T12" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.423
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t8
title: "Table_T08" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.259
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t9
title: "Table_T09" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= 0.087
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t11
title: "Table_T11" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.259
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t13
title: "Table_T13" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.574
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t14
title: "Table_T14" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.707
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.