cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.158037.v1/t9
title: "Figure 3 (lower left)" of "Search for dark matter produced in association with a Higgs boson decaying to a $\tau$ lepton pair in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $95\%$ CL upper limits on the $\mu$ for 2HDM+a model. Observed and expected $95\%$ CL upper limits on the $\mu$ as functions of $\sin\theta$ using $m_{a}$ = 200 GeV, $m_A$ = 600 GeV, $\tan\beta$ = 1, and $m_\chi$ = 10 GeV. The interpolation between the points is linear.
description: A search for dark matter particles produced in association with a Higgs boson decaying into a pair of $\tau$ leptons is performed using data collected in proton-proton collisions at a center-of-mass energy of 13\TeV with the CMS detector. The analysis is based on a data set corresponding to an integrated luminosity of 101\fbinv collected in 2017--2018. No significant excess over the expected standard model background is observed. This result is interpreted within the framework of the 2HDM+a and baryonic ${\rm Z}^{\prime}$ benchmark simplified models. Upper limits at 95\% confidence level are set on the product of the production cross section and branching fraction in the two simplified models. In the 2HDM+a model, a type-II two-Higgs-doublet model featuring a heavy pseudoscalar with an additional light pseudoscalar, the heavy pseudoscalar boson masses between 400 and 700\GeV are excluded for a light pseudoscalar mass of 100\GeV. For the baryonic ${Z}^{\prime}$ model, a statistical combination is made with an earlier search based on a data set of 36\fbinv collected in 2016. In this model, ${Z}^{\prime}$ boson masses up to 1050\GeV are excluded for a dark matter particle mass of 1\GeV.
DOI: 10.15468/dl.xgke8k
title: Occurrence Download

description: A dataset containing 1261 species occurrences available in GBIF matching the query:
{
 "and" : [
 "BasisOfRecord is Specimen",
 "Continent is North America",
 "Country is United States of America",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "TaxonKey is Reynoutria japonica"
 ]
}

 The dataset includes 1261 records from 129 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0016037-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.158037.v1/t10
title: "Figure 3 (lower right)" of "Search for dark matter produced in association with a Higgs boson decaying to a $\tau$ lepton pair in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $95\%$ CL upper limits on the $\mu$ for 2HDM+a model. Observed and expected $95\%$ CL upper limits on the $\mu$ as functions of $\tan\beta$ using $m_a$ = 150 GeV, $m_A$ = 600 GeV, $\sin\theta$ = 0.35, and $m_\chi$ = 10 GeV. The interpolation between the points is linear.
description: A search for dark matter particles produced in association with a Higgs boson decaying into a pair of $\tau$ leptons is performed using data collected in proton-proton collisions at a center-of-mass energy of 13\TeV with the CMS detector. The analysis is based on a data set corresponding to an integrated luminosity of 101\fbinv collected in 2017--2018. No significant excess over the expected standard model background is observed. This result is interpreted within the framework of the 2HDM+a and baryonic ${\rm Z}^{\prime}$ benchmark simplified models. Upper limits at 95\% confidence level are set on the product of the production cross section and branching fraction in the two simplified models. In the 2HDM+a model, a type-II two-Higgs-doublet model featuring a heavy pseudoscalar with an additional light pseudoscalar, the heavy pseudoscalar boson masses between 400 and 700\GeV are excluded for a light pseudoscalar mass of 100\GeV. For the baryonic ${Z}^{\prime}$ model, a statistical combination is made with an earlier search based on a data set of 36\fbinv collected in 2016. In this model, ${Z}^{\prime}$ boson masses up to 1050\GeV are excluded for a dark matter particle mass of 1\GeV.
DOI: 10.17182/hepdata.158037.v1/t11
title: "Figure 4" of "Search for dark matter produced in association with a Higgs boson decaying to a $\tau$ lepton pair in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $95\%$ CL upper limits on the $\mu$ in the $m_a-m_A$ plane for 2HDM+a model. The regions inside the red and black curves correspond to the observed and expected exclusions at $95\%$ CL, respectively.
description: A search for dark matter particles produced in association with a Higgs boson decaying into a pair of $\tau$ leptons is performed using data collected in proton-proton collisions at a center-of-mass energy of 13\TeV with the CMS detector. The analysis is based on a data set corresponding to an integrated luminosity of 101\fbinv collected in 2017--2018. No significant excess over the expected standard model background is observed. This result is interpreted within the framework of the 2HDM+a and baryonic ${\rm Z}^{\prime}$ benchmark simplified models. Upper limits at 95\% confidence level are set on the product of the production cross section and branching fraction in the two simplified models. In the 2HDM+a model, a type-II two-Higgs-doublet model featuring a heavy pseudoscalar with an additional light pseudoscalar, the heavy pseudoscalar boson masses between 400 and 700\GeV are excluded for a light pseudoscalar mass of 100\GeV. For the baryonic ${Z}^{\prime}$ model, a statistical combination is made with an earlier search based on a data set of 36\fbinv collected in 2016. In this model, ${Z}^{\prime}$ boson masses up to 1050\GeV are excluded for a dark matter particle mass of 1\GeV.
DOI: 10.17182/hepdata.158037.v1/t12
title: "Figure 5 (left)" of "Search for dark matter produced in association with a Higgs boson decaying to a $\tau$ lepton pair in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $95\%$ CL upper limits on the $\mu$ for baryonic Z' model. Observed and expected $95\%$ CL upper limits on the $\mu$ as a function of $m_{Z'}$, using $m_{\chi}$ = 1 GeV. The interpolation between the points is linear.
description: A search for dark matter particles produced in association with a Higgs boson decaying into a pair of $\tau$ leptons is performed using data collected in proton-proton collisions at a center-of-mass energy of 13\TeV with the CMS detector. The analysis is based on a data set corresponding to an integrated luminosity of 101\fbinv collected in 2017--2018. No significant excess over the expected standard model background is observed. This result is interpreted within the framework of the 2HDM+a and baryonic ${\rm Z}^{\prime}$ benchmark simplified models. Upper limits at 95\% confidence level are set on the product of the production cross section and branching fraction in the two simplified models. In the 2HDM+a model, a type-II two-Higgs-doublet model featuring a heavy pseudoscalar with an additional light pseudoscalar, the heavy pseudoscalar boson masses between 400 and 700\GeV are excluded for a light pseudoscalar mass of 100\GeV. For the baryonic ${Z}^{\prime}$ model, a statistical combination is made with an earlier search based on a data set of 36\fbinv collected in 2016. In this model, ${Z}^{\prime}$ boson masses up to 1050\GeV are excluded for a dark matter particle mass of 1\GeV.
DOI: 10.17182/hepdata.158037.v1/t13
title: "Figure 5 (right)" of "Search for dark matter produced in association with a Higgs boson decaying to a $\tau$ lepton pair in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The $95\%$ CL upper limits on the $\mu$ for baryonic Z' model. $95\%$ CL upper limits on the $\mu$ in $m_{Z'}-m_{\chi}$ plane. The regions inside the red and black curve correspond to the observed and expected exclusions at $95\%$ CL, respectively.
description: A search for dark matter particles produced in association with a Higgs boson decaying into a pair of $\tau$ leptons is performed using data collected in proton-proton collisions at a center-of-mass energy of 13\TeV with the CMS detector. The analysis is based on a data set corresponding to an integrated luminosity of 101\fbinv collected in 2017--2018. No significant excess over the expected standard model background is observed. This result is interpreted within the framework of the 2HDM+a and baryonic ${\rm Z}^{\prime}$ benchmark simplified models. Upper limits at 95\% confidence level are set on the product of the production cross section and branching fraction in the two simplified models. In the 2HDM+a model, a type-II two-Higgs-doublet model featuring a heavy pseudoscalar with an additional light pseudoscalar, the heavy pseudoscalar boson masses between 400 and 700\GeV are excluded for a light pseudoscalar mass of 100\GeV. For the baryonic ${Z}^{\prime}$ model, a statistical combination is made with an earlier search based on a data set of 36\fbinv collected in 2016. In this model, ${Z}^{\prime}$ boson masses up to 1050\GeV are excluded for a dark matter particle mass of 1\GeV.
DOI: 10.17182/hepdata.158065.v1/t1
title: "Table 1" of "Systematic study of flow vector decorrelation in $\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02}$ TeV Pb-Pb collisions"

description: The ratio $v_{2}{2}/v_2[2]$ as a function of $p_{\rm T}$ in different centrality intervals
description: Measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations at $\sqrt{s_\mathrm{NN}} = 5.02$ with two-particle correlations. Significant $p_\mathrm{T}$-dependent fluctuations of the $\vec{V}_{2}$ flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to $\sim$15\% being present in the 5\% most central collisions. In parallel, no evidence of significant $p_\mathrm{T}$-dependent fluctuations of $\vec{V}_{3}$ or $\vec{V}_{4}$ is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than $5\sigma$ significance in central collisions. These observations in Pb-Pb collisions indicate precisely where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high $p_\mathrm{T}$, which are biased by kinematic-dependent fluctuations of the flow vector direction of at least 23\% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system.
DOI: 10.17182/hepdata.158065.v1/t2
title: "Table 2" of "Systematic study of flow vector decorrelation in $\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02}$ TeV Pb-Pb collisions"

description: The ratio $v_{3}{2}/v_3[2]$ as a function of $p_{\rm T}$ in different centrality intervals
description: Measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations at $\sqrt{s_\mathrm{NN}} = 5.02$ with two-particle correlations. Significant $p_\mathrm{T}$-dependent fluctuations of the $\vec{V}_{2}$ flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to $\sim$15\% being present in the 5\% most central collisions. In parallel, no evidence of significant $p_\mathrm{T}$-dependent fluctuations of $\vec{V}_{3}$ or $\vec{V}_{4}$ is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than $5\sigma$ significance in central collisions. These observations in Pb-Pb collisions indicate precisely where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high $p_\mathrm{T}$, which are biased by kinematic-dependent fluctuations of the flow vector direction of at least 23\% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system.
DOI: 10.17182/hepdata.158065.v1/t3
title: "Table 3" of "Systematic study of flow vector decorrelation in $\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02}$ TeV Pb-Pb collisions"

description: The ratio $v_{4}{2}/v_4[2]$ as a function of $p_{\rm T}$ in different centrality intervals
description: Measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations at $\sqrt{s_\mathrm{NN}} = 5.02$ with two-particle correlations. Significant $p_\mathrm{T}$-dependent fluctuations of the $\vec{V}_{2}$ flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to $\sim$15\% being present in the 5\% most central collisions. In parallel, no evidence of significant $p_\mathrm{T}$-dependent fluctuations of $\vec{V}_{3}$ or $\vec{V}_{4}$ is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than $5\sigma$ significance in central collisions. These observations in Pb-Pb collisions indicate precisely where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high $p_\mathrm{T}$, which are biased by kinematic-dependent fluctuations of the flow vector direction of at least 23\% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system.
DOI: 10.5281/zenodo.17527342
title: City Bike Counts (Synthetic) — September 2025

description: Daily counts of bicycle check-ins at three city stations over 30 days (2025-09-01 to 2025-09-30). Synthetic dataset for demonstrating data curation and repository deposit workflows.
DOI: 10.5281/zenodo.17527372
title: City Bike Counts (Synthetic) — September 2025

description: Daily counts of bicycle check-ins at three city stations over 30 days (2025-09-01 to 2025-09-30). Synthetic dataset for demonstrating data curation and repository deposit workflows.
DOI: 10.17182/hepdata.158065.v1/t10
title: "Table 10" of "Systematic study of flow vector decorrelation in $\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02}$ TeV Pb-Pb collisions"

description: The factorization ratio $r_{3}$ as a function of $p_{\rm T}^{\rm a}$ for different $p_{\rm T}^{\rm t}$ intervals in 40-50% centrality
description: Measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations at $\sqrt{s_\mathrm{NN}} = 5.02$ with two-particle correlations. Significant $p_\mathrm{T}$-dependent fluctuations of the $\vec{V}_{2}$ flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to $\sim$15\% being present in the 5\% most central collisions. In parallel, no evidence of significant $p_\mathrm{T}$-dependent fluctuations of $\vec{V}_{3}$ or $\vec{V}_{4}$ is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than $5\sigma$ significance in central collisions. These observations in Pb-Pb collisions indicate precisely where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high $p_\mathrm{T}$, which are biased by kinematic-dependent fluctuations of the flow vector direction of at least 23\% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system.
DOI: 10.17182/hepdata.158065.v1/t4
title: "Table 4" of "Systematic study of flow vector decorrelation in $\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02}$ TeV Pb-Pb collisions"

description: The factorization ratio $r_{2}$ as a function of $p_{\rm T}^{\rm a}$ for different $p_{\rm T}^{\rm t}$ intervals in 0-5% centrality
description: Measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations at $\sqrt{s_\mathrm{NN}} = 5.02$ with two-particle correlations. Significant $p_\mathrm{T}$-dependent fluctuations of the $\vec{V}_{2}$ flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to $\sim$15\% being present in the 5\% most central collisions. In parallel, no evidence of significant $p_\mathrm{T}$-dependent fluctuations of $\vec{V}_{3}$ or $\vec{V}_{4}$ is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than $5\sigma$ significance in central collisions. These observations in Pb-Pb collisions indicate precisely where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high $p_\mathrm{T}$, which are biased by kinematic-dependent fluctuations of the flow vector direction of at least 23\% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system.
DOI: 10.17182/hepdata.158065.v1/t5
title: "Table 5" of "Systematic study of flow vector decorrelation in $\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02}$ TeV Pb-Pb collisions"

description: The factorization ratio $r_{2}$ as a function of $p_{\rm T}^{\rm a}$ for different $p_{\rm T}^{\rm t}$ intervals in 20-30% centrality
description: Measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations at $\sqrt{s_\mathrm{NN}} = 5.02$ with two-particle correlations. Significant $p_\mathrm{T}$-dependent fluctuations of the $\vec{V}_{2}$ flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to $\sim$15\% being present in the 5\% most central collisions. In parallel, no evidence of significant $p_\mathrm{T}$-dependent fluctuations of $\vec{V}_{3}$ or $\vec{V}_{4}$ is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than $5\sigma$ significance in central collisions. These observations in Pb-Pb collisions indicate precisely where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high $p_\mathrm{T}$, which are biased by kinematic-dependent fluctuations of the flow vector direction of at least 23\% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system.
DOI: 10.17182/hepdata.158065.v1/t6
title: "Table 6" of "Systematic study of flow vector decorrelation in $\mathbf{\sqrt{\textit{s}_{_{\bf NN}}}=5.02}$ TeV Pb-Pb collisions"

description: The factorization ratio $r_{2}$ as a function of $p_{\rm T}^{\rm a}$ for different $p_{\rm T}^{\rm t}$ intervals in 40-50% centrality
description: Measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the $p_\mathrm{T}$-dependent flow vector fluctuations at $\sqrt{s_\mathrm{NN}} = 5.02$ with two-particle correlations. Significant $p_\mathrm{T}$-dependent fluctuations of the $\vec{V}_{2}$ flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to $\sim$15\% being present in the 5\% most central collisions. In parallel, no evidence of significant $p_\mathrm{T}$-dependent fluctuations of $\vec{V}_{3}$ or $\vec{V}_{4}$ is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than $5\sigma$ significance in central collisions. These observations in Pb-Pb collisions indicate precisely where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high $p_\mathrm{T}$, which are biased by kinematic-dependent fluctuations of the flow vector direction of at least 23\% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system.