cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.102570.v1/t8
title: "Table 29-32" of "Measurement of charged particle multiplicity distributions in DIS at HERA and its implication to entanglement entropy of partons"

description: KNO function for charged particles neasured with the additional restriction to select only particles from the current region of the Breit frame $0&lt;\eta^{*}&lt;4$, in 4x4 kinematic bins of $Q^2$ and $y$.
description: H1 collaboration Eur.Phys.J.C81 (2021), 212, [arxiv:2011.01812]. Charged particle multiplicity distribution $P(N)$ measured in deep-inelastic scattering at HERA as a function of the number of charged particles $N$ in the pseudorapidity range $\vert\eta_{lab}\vert&lt;1.6$ for transverse momenta $P_{T,lab}&gt;150$ MeV. The data are binned into a two-dimensional grid of size 4x4 in momentum transfer $Q^2$ and inelasticity $y$. For some of the measurements the bins in $y$ are translated to the equivalent hadronic energy $W$ or to Bjorken-x. The measurements are repeated for three subregions in the track psedorapidity and further with a restriction to the current regioon of the Breit frame, $0&lt;\eta^{*}&lt;4$. The analyzed kinematic range is $5
DOI: 10.17182/hepdata.102570.v1/t9
title: "Table 7" of "Measurement of charged particle multiplicity distributions in DIS at HERA and its implication to entanglement entropy of partons"

description: Hadron entropy for charged particles selected in a sliding pseudorapidity window of 1.4 units size with transverse momenta $P_{T lab}&gt;150$ MeV, in the accessible kinematic bins of momentum transfer $Q^2$ and $y$. The data are presented as a function of $Q^2$ and the corresponding average $x$-Bjorken.
description: H1 collaboration Eur.Phys.J.C81 (2021), 212, [arxiv:2011.01812]. Charged particle multiplicity distribution $P(N)$ measured in deep-inelastic scattering at HERA as a function of the number of charged particles $N$ in the pseudorapidity range $\vert\eta_{lab}\vert&lt;1.6$ for transverse momenta $P_{T,lab}&gt;150$ MeV. The data are binned into a two-dimensional grid of size 4x4 in momentum transfer $Q^2$ and inelasticity $y$. For some of the measurements the bins in $y$ are translated to the equivalent hadronic energy $W$ or to Bjorken-x. The measurements are repeated for three subregions in the track psedorapidity and further with a restriction to the current regioon of the Breit frame, $0&lt;\eta^{*}&lt;4$. The analyzed kinematic range is $5
DOI: 10.17182/hepdata.102570.v1/t10
title: "Table 8" of "Measurement of charged particle multiplicity distributions in DIS at HERA and its implication to entanglement entropy of partons"

description: Hadron entropy for charged particles neasured with the additional restriction to select only particles from the current region of the Breit frame $0&lt;\eta^{*}&lt;4$, in 4x4 kinematic bins of $Q^2$ and $y$. The data are presented as a function of $Q^2$ and the corresponding average $x$-Bjorken.
description: H1 collaboration Eur.Phys.J.C81 (2021), 212, [arxiv:2011.01812]. Charged particle multiplicity distribution $P(N)$ measured in deep-inelastic scattering at HERA as a function of the number of charged particles $N$ in the pseudorapidity range $\vert\eta_{lab}\vert&lt;1.6$ for transverse momenta $P_{T,lab}&gt;150$ MeV. The data are binned into a two-dimensional grid of size 4x4 in momentum transfer $Q^2$ and inelasticity $y$. For some of the measurements the bins in $y$ are translated to the equivalent hadronic energy $W$ or to Bjorken-x. The measurements are repeated for three subregions in the track psedorapidity and further with a restriction to the current regioon of the Breit frame, $0&lt;\eta^{*}&lt;4$. The analyzed kinematic range is $5
DOI: 10.17182/hepdata.95747.v1/t1
title: "Differential diphoton invariant mass" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for diphoton invariant mass are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line) with bands denoting the theoretical uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.95747.v1/t2
title: "Differential normalised diphoton invariant mass" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured normalised differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for diphoton invariant mass are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line).
description: No data abstract available.
DOI: 10.17182/hepdata.95747.v1/t3
title: "Differential diphoton $|cos(\theta*)|$" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for diphoton $|cos(\theta*)|$ are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line) with bands denoting the theoretical uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.95747.v1/t4
title: "Differential normalised diphoton $|cos(\theta*)|$" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured normalised differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for diphoton $|cos(\theta*)|$ are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line).
description: No data abstract available.
DOI: 10.17182/hepdata.95747.v1/t5
title: "Differential average photon transverse momentum" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured normalised differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for average photon transverse momentum are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line) with bands denoting the theoretical uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.94802.v1/t1
title: "Table 1" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from MBT events plotted as a function of the A-particle $p_\mathrm{T}$ for 0-5% centrality.
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t2
title: "Table 2" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from $p_{T}^{jet}&gt;75$ GeV events plotted as a function of the A-particle $p_\mathrm{T}$ for 0-5% centrality.
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t3
title: "Table 3" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from $p_{T}^{jet}&gt;100$ GeV events plotted as a function of the A-particle $p_\mathrm{T}$ for 0-5% centrality.
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t4
title: "Table 4" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{3}$ from MBT events plotted as a function of the A-particle $p_\mathrm{T}$ for 0-5% centrality.
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.95747.v1/t6
title: "Differential normalised average photon transverse momentum" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured normalised differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for average photon transverse momentum are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line).
description: No data abstract available.
DOI: 10.17182/hepdata.95747.v1/t7
title: "Differential diphoton rapidity" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for diphoton rapidity are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line) with bands denoting the theoretical uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.95747.v1/t8
title: "Differential normalised diphoton rapidity" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: Measured normalised differential fiducial cross sections of $\gamma\gamma \rightarrow \gamma\gamma$ production in Pb+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV for diphoton rapidity are shown as points with error bars giving the statistical uncertainty and grey bands indicating the size of the total uncertainty. The results are compared with the prediction from the SuperChic v3.0 MC generator (solid line).
description: No data abstract available.
DOI: 10.17182/hepdata.94802.v1/t5
title: "Table 5" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{3}$ from $p_{T}^{jet}&gt;75$ GeV events plotted as a function of the A-particle $p_\mathrm{T}$ for 0-5% centrality.
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t6
title: "Table 6" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{3}$ from $p_{T}^{jet}&gt;100$ GeV events plotted as a function of the A-particle $p_\mathrm{T}$ for 0-5% centrality.
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t7
title: "Table 7" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from MBT events plotted as a function of the event centrality and A-particle $p_\mathrm{T}$ in (0.5-2 GeV).
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t8
title: "Table 8" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from $p_{T}^{jet}&gt;75$ GeV events plotted as a function of the event centrality and A-particle $p_\mathrm{T}$ in (0.5-2 GeV).
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.95747.v1/t10
title: "The 95% CL upper limit on the ALP coupling $1/\Lambda_{a}$" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: The 95% CL upper limit on the ALP coupling $1/\Lambda_{a}$ for the $\gamma\gamma\rightarrow a \rightarrow \gamma\gamma$ process as a function of ALP mass m$_{a}$. The observed upper limit is shown as a solid black line and the expected upper limit is shown by the dashed black line with its $\pm1$ and $\pm2$ standard deviation bands. The discontinuity at $m_{a} = 70 GeV$ is caused by the increase of the mass-bin width which brings an increase in signal acceptance.
description: No data abstract available.
DOI: 10.17182/hepdata.95747.v1/t9
title: "The 95% CL upper limit on the ALP cross section" of "Measurement of light-by-light scattering and search for axion-like particles with 2.2 nb$^{-1}$ of Pb+Pb data with the ATLAS detector"

description: The 95% CL upper limit on the ALP cross section $\sigma_{\gamma\gamma\rightarrow a \rightarrow\gamma\gamma}$ for the $\gamma\gamma\rightarrow a \rightarrow \gamma\gamma$ process as a function of ALP mass m$_{a}$. The observed upper limit is shown as a solid black line and the expected upper limit is shown by the dashed black line with its $\pm1$ and $\pm2$ standard deviation bands. The discontinuity at $m_{a}=70 GeV$ is caused by the increase of the mass-bin width which brings an increase in signal acceptance.
description: No data abstract available.
DOI: 10.15468/dl.tmwjd2
title: Occurrence Download

description: A dataset containing 113 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Cassia roxburghii",
 "HasCoordinate is true",
 "OccurrenceStatus is Present",
 {
 "not" : {
 "BasisOfRecord" : [
 "is Fossil"
 ]
 }
 }
 ]
}

 The dataset includes 113 records from 24 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0003996-260208012135463/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.94802.v1/t10
title: "Table 10" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from MBT events plotted as a function of the event centrality and A-particle $p_\mathrm{T}$ in (2-9 GeV).
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t11
title: "Table 11" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from $p_{T}^{jet}&gt;75$ GeV events plotted as a function of the event centrality and A-particle $p_\mathrm{T}$ in (2-9 GeV).
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.
DOI: 10.17182/hepdata.94802.v1/t12
title: "Table 12" of "Transverse momentum and process dependent azimuthal anisotropies in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions with the ATLAS detector"

description: Distribution of $v_{2}$ from $p_{T}^{jet}&gt;100$ GeV events plotted as a function of the event centrality and A-particle $p_\mathrm{T}$ in (2-9 GeV).
description: The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{−1}$ recorded in 2016. The results are shown as a function of particle $p_\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\mathrm{T}$ jet; this selection enhances the statistics of high $p_\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.