cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.159627.v1/t7
title: "Response matrix pp" of "Probing early parton emissions in heavy ion collisions using the Lund jet plane"

description: The response matrix used for the unfolding of the pp collision data. The binning of the reconstruction (truth) level is divided into 2 (4) large blocks of pt with binning (100-)185-200-1000(1200), divided into blocks of different kt with binning (0-)3-5-10-20-40(-70), divided into $ln(1/\Delta)$ with binning (0.01-)0.916291-1.04982-1.20397-1.30933-1.60944-1.96611-2.30258-2.58279-2.91609-3.24939-3.91599-4.24929(-10). The bins situated outside of the Lund plane at angle 3.91599-4.24929 and kT of 20-40 GeV represent the number of jets in the corresponding pT range.
description: The first relative transverse momentum ($k_{\text{T}}$) scan of the Lund jet plane of high-energy jets produced in lead-lead (PbPb) collisions is presented and compared to the result obtained in proton-proton (pp) collisions. The PbPb (pp) data were recorded by the CMS experiment in 2018 (2017) and correspond to an integrated luminosity of $1.7$ nb$^{-1}$ ($301$ pb$^{-1}$) at a nucleon-nucleon center-of-mass energy of 5.02 TeV. The angular distribution of the primary emissions with the highest $k_{\text{T}}$ of anti-$k_{\text{T}}$ jets with a distance parameter $R=0.4$ is reported. Two different ranges of $k_{\text{T}}$ are investigated for jets with transverse momentum in the range $200 &lt; p_{\text{T}}^\text{jet} &lt; 1000$ GeV, in order to explore the energy scale dependence of the jet quenching phenomena.The measurement was designed to test whether the earliest jet emissions are produced before the formation of the quark-gluon plasma in PbPb collisions.The angular distribution of emissions at high $k_{\text{T}}$ has a similar shape in pp and PbPb collisions, which is consistent with the emissions being part of the early and vacuum-like regime of the jet evolution in PbPb collisions.
DOI: 10.15468/dl.5d45fc
title: Occurrence Download

description: A dataset containing 4785 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (, , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , Erechtites valerianifolius, , , , , , , , , , , , , , , , , , , , , , , , , , , , , , Erechtites valerianifolia, , Erechtites valerianifolia, , Metapocyrtus dagtum, , , , Senecio valerianifolius, , , Senecio valerianifolius, Senecio crassus, Senecio valerianifolius, , , , , , , , , , Senecio palustris, , , , , , , , , , , , , , , , , , , , , , , Senecio valerianaefolius, Senecio valerianifolius, , , , , , , , , , , , , , , , , , , , Erechtites valerianaefolia, Senecio paludicola, Eupatorium angosturae, Gynura rosea, Senecio valerianifolius, , , , , , , , , Crassocephalum valerianifolium, Erechtites gardnerianus, , , Erechtites ambigua, , , , , , , , , , , , , , , , , , , , , , , , , , , , Erechtites organensis, Erechtites ambiguus, Sonchus erythropappus, , , , , , , , , , , , , Senecio valerianifolius, , , , , )",
 "BasisOfRecord is one of (Specimen, Human Observation, Observation, Living Specimen, Machine Observation, Literature Occurrence)",
 "Geometry POLYGON((-180 -90,180 -90,180 90,-180 90,-180 -90))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 4785 records from 236 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0004478-260226173443078/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.5281/zenodo.18816617
title: ENTRE A MEDIAÇÃO E O PODER: MÍDIAS, MEMÓRIA SOCIAL E RECONFIGURAÇÕES DA CULTURA POLÍTICA NA SOCIEDADE COMTEMPÔRANEA

description: Este projeto de pesquisa investiga as complexas relações entre as mídias, a memória social e a cultura política na sociedade contemporânea. Com fundamentação na História Política e na História do Tempo Presente, o estudo analisa como as mídias atuam como agentes ativos na construção de narrativas e na conformação de identidades coletivas. A investigação utiliza referenciais teóricos de Pierre Bourdieu, Michel Foucault e Roger Chartier para compreender o poder simbólico e os processos de mediação no espaço público brasileiro entre o final do século XX e o início do século XXI.

Projeto de pesquisa original com densa fundamentação teórica em História e Geopolítica, focado nas dinâmicas de poder e mediação sociocultural
DOI: 10.5281/zenodo.18816616
title: ENTRE A MEDIAÇÃO E O PODER: MÍDIAS, MEMÓRIA SOCIAL E RECONFIGURAÇÕES DA CULTURA POLÍTICA NA SOCIEDADE COMTEMPÔRANEA

description: Este projeto de pesquisa investiga as complexas relações entre as mídias, a memória social e a cultura política na sociedade contemporânea. Com fundamentação na História Política e na História do Tempo Presente, o estudo analisa como as mídias atuam como agentes ativos na construção de narrativas e na conformação de identidades coletivas. A investigação utiliza referenciais teóricos de Pierre Bourdieu, Michel Foucault e Roger Chartier para compreender o poder simbólico e os processos de mediação no espaço público brasileiro entre o final do século XX e o início do século XXI.

Projeto de pesquisa original com densa fundamentação teórica em História e Geopolítica, focado nas dinâmicas de poder e mediação sociocultural
DOI: 10.15468/2wlj2m
title: Academy of Natural Sciences of Philadelphia Herpetology Collection

description: (placeholder)
DOI: 10.17182/hepdata.168219.v1/t2
title: "Table 2" of "Observation of the jet diffusion wake using dijets in heavy ion collisions"

description: The difference of the near-side charged-particle yields $\mathrm{R^{asym}}-\mathrm{R^{sym}}$ in the charged-particles transverse momentum range $2 &lt; p^{\mathrm{ch}}_{\mathrm{T}} &lt; 4$ GeV as a function of $\Delta\eta^{\mathrm{ch}, \mathrm{jet}_{1}}$ in pp and $0-30\%$, $30-50\%$, and $50-80\%$ PbPb collisions.
description: Energetic quarks and gluons traversing a hot and dense quark-gluon plasma deposit energy and momentum into the medium before hadronizing to collimated sprays of particles, known as jets. This energy-momentum deposition is expected to produce medium responses, collectively known as jet wakes, with "diffusion wake" denoting a depletion of particles in the direction opposite to the propagating jet. These phenomena are studied by comparing dijet-hadron correlations measured in lead-lead (PbPb) and proton-proton (pp) collisions to assess jet-induced modifications of bulk particle production. The analysis uses PbPb and pp data recorded at a nucleon-nucleon center-of-mass energy $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ with the CMS detector at the CERN LHC. By exploring how the dijet-hadron correlation distributions differ for various pseudorapidity separations of the two jets in the dijet, the presence of a jet diffusion wake is firmly established. The wake has a significance greater than 5 standard deviations for charged particles in the transverse momentum range $1 &lt; p_{\mathrm{T}} &lt; 2$ GeV. The measurements are compared with various model predictions with and without jet wake effects, providing new insights into quark-gluon plasma properties and the formation of jet-induced wakes.
DOI: 10.17182/hepdata.168219.v1/t4
title: "Table 4" of "Observation of the jet diffusion wake using dijets in heavy ion collisions"

description: Charged-particle yield difference integrated over $-2.4 &lt; \Delta\eta^{\mathrm{ch}, \mathrm{jet}_{1}} &lt; -0.6$ as a function of PbPb collision centrality for the charged-particle transverse momentum ranges $1 &lt; p^{\mathrm{ch}}_{\mathrm{T}} &lt; 2$ GeV and $2 &lt; p^{\mathrm{ch}}_{\mathrm{T}} &lt; 4$ GeV.
description: Energetic quarks and gluons traversing a hot and dense quark-gluon plasma deposit energy and momentum into the medium before hadronizing to collimated sprays of particles, known as jets. This energy-momentum deposition is expected to produce medium responses, collectively known as jet wakes, with "diffusion wake" denoting a depletion of particles in the direction opposite to the propagating jet. These phenomena are studied by comparing dijet-hadron correlations measured in lead-lead (PbPb) and proton-proton (pp) collisions to assess jet-induced modifications of bulk particle production. The analysis uses PbPb and pp data recorded at a nucleon-nucleon center-of-mass energy $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ with the CMS detector at the CERN LHC. By exploring how the dijet-hadron correlation distributions differ for various pseudorapidity separations of the two jets in the dijet, the presence of a jet diffusion wake is firmly established. The wake has a significance greater than 5 standard deviations for charged particles in the transverse momentum range $1 &lt; p_{\mathrm{T}} &lt; 2$ GeV. The measurements are compared with various model predictions with and without jet wake effects, providing new insights into quark-gluon plasma properties and the formation of jet-induced wakes.
DOI: 10.17182/hepdata.168219.v1/t1
title: "Table 1" of "Observation of the jet diffusion wake using dijets in heavy ion collisions"

description: The difference of the near-side charged-particle yields $\mathrm{R^{asym}}-\mathrm{R^{sym}}$ in the charged-particles transverse momentum range $1 &lt; p^{\mathrm{ch}}_{\mathrm{T}} &lt; 2$ GeV as a function of $\Delta\eta^{\mathrm{ch}, \mathrm{jet}_{1}}$ in pp and $0-30\%$, $30-50\%$, and $50-80\%$ PbPb collisions.
description: Energetic quarks and gluons traversing a hot and dense quark-gluon plasma deposit energy and momentum into the medium before hadronizing to collimated sprays of particles, known as jets. This energy-momentum deposition is expected to produce medium responses, collectively known as jet wakes, with "diffusion wake" denoting a depletion of particles in the direction opposite to the propagating jet. These phenomena are studied by comparing dijet-hadron correlations measured in lead-lead (PbPb) and proton-proton (pp) collisions to assess jet-induced modifications of bulk particle production. The analysis uses PbPb and pp data recorded at a nucleon-nucleon center-of-mass energy $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ with the CMS detector at the CERN LHC. By exploring how the dijet-hadron correlation distributions differ for various pseudorapidity separations of the two jets in the dijet, the presence of a jet diffusion wake is firmly established. The wake has a significance greater than 5 standard deviations for charged particles in the transverse momentum range $1 &lt; p_{\mathrm{T}} &lt; 2$ GeV. The measurements are compared with various model predictions with and without jet wake effects, providing new insights into quark-gluon plasma properties and the formation of jet-induced wakes.
DOI: 10.17182/hepdata.168219.v1/t3
title: "Table 3" of "Observation of the jet diffusion wake using dijets in heavy ion collisions"

description: Particle yield differences $\mathrm{R^{asym}}-\mathrm{R^{sym}}$ as a function of $\Delta\eta^{\mathrm{ch}, \mathrm{jet}_{1}}$ for central $(0-30\%)$ PbPb collisions. The results correspond to the charged-particle transverse momentum range $1 &lt; p^{\mathrm{ch}}_{\mathrm{T}} &lt; 2$ GeV for $\mathrm{R^{asym}}$ with $\Delta\eta^{\mathrm{jet}_{1}, \mathrm{jet}_{2}} \in (0.5, 1.0)$, $\Delta\eta^{\mathrm{jet}_{1}, \mathrm{jet}_{2}} \in (1.0, 1.5)$, and $\Delta\eta^{\mathrm{jet}_{1}, \mathrm{jet}_{2}} \in (1.5, 2.0)$. The result for $2 &lt; p^{\mathrm{ch}}_{\mathrm{T}} &lt; 4$ GeV corresponds to $\mathrm{R^{asym}}$ with $\Delta\eta^{\mathrm{jet}_{1}, \mathrm{jet}_{2}} \in (1.0, 1.5)$.
description: Energetic quarks and gluons traversing a hot and dense quark-gluon plasma deposit energy and momentum into the medium before hadronizing to collimated sprays of particles, known as jets. This energy-momentum deposition is expected to produce medium responses, collectively known as jet wakes, with "diffusion wake" denoting a depletion of particles in the direction opposite to the propagating jet. These phenomena are studied by comparing dijet-hadron correlations measured in lead-lead (PbPb) and proton-proton (pp) collisions to assess jet-induced modifications of bulk particle production. The analysis uses PbPb and pp data recorded at a nucleon-nucleon center-of-mass energy $\sqrt{s_{_{\mathrm{NN}}}} = 5.02$ with the CMS detector at the CERN LHC. By exploring how the dijet-hadron correlation distributions differ for various pseudorapidity separations of the two jets in the dijet, the presence of a jet diffusion wake is firmly established. The wake has a significance greater than 5 standard deviations for charged particles in the transverse momentum range $1 &lt; p_{\mathrm{T}} &lt; 2$ GeV. The measurements are compared with various model predictions with and without jet wake effects, providing new insights into quark-gluon plasma properties and the formation of jet-induced wakes.
DOI: 10.15468/dl.vz336c
title: Occurrence Download

description: A dataset containing 48 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Tropidolaemus philippensis"
 ]
}

 The dataset includes 48 records from 12 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0004479-260226173443078/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.168218.v1/t2
title: "NeNe RAA (fine pT binning)" of "System-size dependence of charged-particle suppression in ultrarelativistic nucleus-nucleus collisions"

description: Charged-particle nuclear modification factor in NeNe collisions.
description: High-energy partons lose energy while propagating through the hot, strongly interacting medium produced in ultrarelativistic nucleus-nucleus collisions, leading to a suppression of particle production at high transverse momentum ($p_\mathrm{T}$). The dependence of this energy loss on the size of the colliding nuclear system has yet to be firmly established experimentally. This Letter presents a systematic study of charged-particle suppression across four different nucleus-nucleus collision systems using nuclear modification factors ($R_\mathrm{AA}$) measured by the CMS Collaboration at the CERN LHC. Previous CMS measurements of $R_\mathrm{AA}$ in oxygen-oxygen, xenon-xenon, and lead-lead collisions are recast with identical $p_\mathrm{T}$ intervals and are complemented by the first measurement of the charged-particle $R_\mathrm{AA}$ in neon-neon collisions at $\sqrt{s}_mathrm{NN} = 5.36$TeV. The neon-neon data correspond to an integrated luminosity of 0.76 nb$^{-1}$. The $R_\mathrm{AA}$ in all collision systems examined show similar qualitative trends, following an ordering with the nucleon number $A$. The $R_\mathrm{AA}$ feature a downward slope at low $p_\mathrm{T}$, a local minimum at around 5--7 GeV, and an upward slope with increasing $p_\mathrm{T}$. The $R_\mathrm{AA}$ are also compared in terms of $A^{1/3}$, which is proportional to the nuclear radius. Models including only initial-state nuclear effects fail to reproduce the observed trends, whereas energy loss models reproduce the trends at high $p_\mathrm{T}$ ($p_\mathrm{T} &gt; 9.6$GeV).
DOI: 10.17182/hepdata.168218.v1/t4
title: "NeNe RAA (coarse pT binning)" of "System-size dependence of charged-particle suppression in ultrarelativistic nucleus-nucleus collisions"

description: Charged-particle nuclear modification factor in NeNe collisions.
description: High-energy partons lose energy while propagating through the hot, strongly interacting medium produced in ultrarelativistic nucleus-nucleus collisions, leading to a suppression of particle production at high transverse momentum ($p_\mathrm{T}$). The dependence of this energy loss on the size of the colliding nuclear system has yet to be firmly established experimentally. This Letter presents a systematic study of charged-particle suppression across four different nucleus-nucleus collision systems using nuclear modification factors ($R_\mathrm{AA}$) measured by the CMS Collaboration at the CERN LHC. Previous CMS measurements of $R_\mathrm{AA}$ in oxygen-oxygen, xenon-xenon, and lead-lead collisions are recast with identical $p_\mathrm{T}$ intervals and are complemented by the first measurement of the charged-particle $R_\mathrm{AA}$ in neon-neon collisions at $\sqrt{s}_mathrm{NN} = 5.36$TeV. The neon-neon data correspond to an integrated luminosity of 0.76 nb$^{-1}$. The $R_\mathrm{AA}$ in all collision systems examined show similar qualitative trends, following an ordering with the nucleon number $A$. The $R_\mathrm{AA}$ feature a downward slope at low $p_\mathrm{T}$, a local minimum at around 5--7 GeV, and an upward slope with increasing $p_\mathrm{T}$. The $R_\mathrm{AA}$ are also compared in terms of $A^{1/3}$, which is proportional to the nuclear radius. Models including only initial-state nuclear effects fail to reproduce the observed trends, whereas energy loss models reproduce the trends at high $p_\mathrm{T}$ ($p_\mathrm{T} &gt; 9.6$GeV).
DOI: 10.17182/hepdata.168218.v1/t5
title: "PbPb RAA (coarse pT binning)" of "System-size dependence of charged-particle suppression in ultrarelativistic nucleus-nucleus collisions"

description: Charged-particle nuclear modification factor in PbPb collisions.
description: High-energy partons lose energy while propagating through the hot, strongly interacting medium produced in ultrarelativistic nucleus-nucleus collisions, leading to a suppression of particle production at high transverse momentum ($p_\mathrm{T}$). The dependence of this energy loss on the size of the colliding nuclear system has yet to be firmly established experimentally. This Letter presents a systematic study of charged-particle suppression across four different nucleus-nucleus collision systems using nuclear modification factors ($R_\mathrm{AA}$) measured by the CMS Collaboration at the CERN LHC. Previous CMS measurements of $R_\mathrm{AA}$ in oxygen-oxygen, xenon-xenon, and lead-lead collisions are recast with identical $p_\mathrm{T}$ intervals and are complemented by the first measurement of the charged-particle $R_\mathrm{AA}$ in neon-neon collisions at $\sqrt{s}_mathrm{NN} = 5.36$TeV. The neon-neon data correspond to an integrated luminosity of 0.76 nb$^{-1}$. The $R_\mathrm{AA}$ in all collision systems examined show similar qualitative trends, following an ordering with the nucleon number $A$. The $R_\mathrm{AA}$ feature a downward slope at low $p_\mathrm{T}$, a local minimum at around 5--7 GeV, and an upward slope with increasing $p_\mathrm{T}$. The $R_\mathrm{AA}$ are also compared in terms of $A^{1/3}$, which is proportional to the nuclear radius. Models including only initial-state nuclear effects fail to reproduce the observed trends, whereas energy loss models reproduce the trends at high $p_\mathrm{T}$ ($p_\mathrm{T} &gt; 9.6$GeV).
DOI: 10.17182/hepdata.168218.v1/t1
title: "NeNe charged-particle pT spectrum" of "System-size dependence of charged-particle suppression in ultrarelativistic nucleus-nucleus collisions"

description: Charged-particle transverse momentum spectrum in NeNe collisions.
description: High-energy partons lose energy while propagating through the hot, strongly interacting medium produced in ultrarelativistic nucleus-nucleus collisions, leading to a suppression of particle production at high transverse momentum ($p_\mathrm{T}$). The dependence of this energy loss on the size of the colliding nuclear system has yet to be firmly established experimentally. This Letter presents a systematic study of charged-particle suppression across four different nucleus-nucleus collision systems using nuclear modification factors ($R_\mathrm{AA}$) measured by the CMS Collaboration at the CERN LHC. Previous CMS measurements of $R_\mathrm{AA}$ in oxygen-oxygen, xenon-xenon, and lead-lead collisions are recast with identical $p_\mathrm{T}$ intervals and are complemented by the first measurement of the charged-particle $R_\mathrm{AA}$ in neon-neon collisions at $\sqrt{s}_mathrm{NN} = 5.36$TeV. The neon-neon data correspond to an integrated luminosity of 0.76 nb$^{-1}$. The $R_\mathrm{AA}$ in all collision systems examined show similar qualitative trends, following an ordering with the nucleon number $A$. The $R_\mathrm{AA}$ feature a downward slope at low $p_\mathrm{T}$, a local minimum at around 5--7 GeV, and an upward slope with increasing $p_\mathrm{T}$. The $R_\mathrm{AA}$ are also compared in terms of $A^{1/3}$, which is proportional to the nuclear radius. Models including only initial-state nuclear effects fail to reproduce the observed trends, whereas energy loss models reproduce the trends at high $p_\mathrm{T}$ ($p_\mathrm{T} &gt; 9.6$GeV).
DOI: 10.17182/hepdata.168218.v1/t3
title: "OO RAA (coarse pT binning)" of "System-size dependence of charged-particle suppression in ultrarelativistic nucleus-nucleus collisions"

description: Charged-particle nuclear modification factor in OO collisions.
description: High-energy partons lose energy while propagating through the hot, strongly interacting medium produced in ultrarelativistic nucleus-nucleus collisions, leading to a suppression of particle production at high transverse momentum ($p_\mathrm{T}$). The dependence of this energy loss on the size of the colliding nuclear system has yet to be firmly established experimentally. This Letter presents a systematic study of charged-particle suppression across four different nucleus-nucleus collision systems using nuclear modification factors ($R_\mathrm{AA}$) measured by the CMS Collaboration at the CERN LHC. Previous CMS measurements of $R_\mathrm{AA}$ in oxygen-oxygen, xenon-xenon, and lead-lead collisions are recast with identical $p_\mathrm{T}$ intervals and are complemented by the first measurement of the charged-particle $R_\mathrm{AA}$ in neon-neon collisions at $\sqrt{s}_mathrm{NN} = 5.36$TeV. The neon-neon data correspond to an integrated luminosity of 0.76 nb$^{-1}$. The $R_\mathrm{AA}$ in all collision systems examined show similar qualitative trends, following an ordering with the nucleon number $A$. The $R_\mathrm{AA}$ feature a downward slope at low $p_\mathrm{T}$, a local minimum at around 5--7 GeV, and an upward slope with increasing $p_\mathrm{T}$. The $R_\mathrm{AA}$ are also compared in terms of $A^{1/3}$, which is proportional to the nuclear radius. Models including only initial-state nuclear effects fail to reproduce the observed trends, whereas energy loss models reproduce the trends at high $p_\mathrm{T}$ ($p_\mathrm{T} &gt; 9.6$GeV).