cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.91160.v1/t391
title: "Table 391" of "Measurement of angular and momentum distributions of charged particles within and around jets in Pb+Pb and $pp$ collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV with the ATLAS detector"

description: From Fig 9. Delta_D(pT,r) The differences between charged particle distributions around jets as a function of distance from the jet axis in different centrality intervals of PbPb and pp collisions at 5.02 TeV for different track pT and jet pT ranges.
description: CERN-LHC. Studies of the fragmentation of jets into charged particles in heavy-ion collisions can provide information about the mechanism of jet-quenching by the hot and dense QCD matter created in such collisions, the quark-gluon plasma. This paper presents a measurement of the angular distribution of charged particles around the jet axis in sNN=5.02 TeV Pb+Pb and pp collisions, using the ATLAS detector at the LHC. The Pb+Pb and pp data sets have integrated luminosities of 0.49 nb−1 and 25 pb−1, respectively. The measurement is performed for jets reconstructed with the anti-kt algorithm with radius parameter R=0.4 and is extended to an angular distance of r=0.8 from the jet axis. Results are presented as a function of Pb+Pb collision centrality and distance from the jet axis for charged particles with transverse momenta in the 1−63 GeV range, matched to jets with transverse momenta in the 126−316 GeV range and an absolute value of jet rapidity of less than 1.7. Modifications to the measured distributions are quantified by taking a ratio to the measurements in pp collisions. Yields of charged particles with transverse momenta below 4 GeV are observed to be increasingly enhanced as a function of angular distance from the jet axis, reaching a maximum at r=0.6. Charged particles with transverse momenta above 4 GeV have an enhanced yield in Pb+Pb collisions in the jet core for angular distances up to r=0.05 from the jet axis, with a suppression at larger distances.
DOI: 10.17182/hepdata.59488.v1/t1
title: "Table 1" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The EP Resolution Factor vs. Centrality for n values from2 to 6.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t2
title: "Table 2" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Chi Reolution Factor vs. Centrality for n values from 2 to 6.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t3
title: "Table 3" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The one-dimensional Delta(PHI) correlation function vs Delta(PHI) for |DETARAP| in the range 2 to 5 summed over all n values from 1 to 6.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.91160.v1/t392
title: "Table 392" of "Measurement of angular and momentum distributions of charged particles within and around jets in Pb+Pb and $pp$ collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV with the ATLAS detector"

description: From Fig 9. Delta_D(pT,r) The differences between charged particle distributions around jets as a function of distance from the jet axis in different centrality intervals of PbPb and pp collisions at 5.02 TeV for different track pT and jet pT ranges.
description: CERN-LHC. Studies of the fragmentation of jets into charged particles in heavy-ion collisions can provide information about the mechanism of jet-quenching by the hot and dense QCD matter created in such collisions, the quark-gluon plasma. This paper presents a measurement of the angular distribution of charged particles around the jet axis in sNN=5.02 TeV Pb+Pb and pp collisions, using the ATLAS detector at the LHC. The Pb+Pb and pp data sets have integrated luminosities of 0.49 nb−1 and 25 pb−1, respectively. The measurement is performed for jets reconstructed with the anti-kt algorithm with radius parameter R=0.4 and is extended to an angular distance of r=0.8 from the jet axis. Results are presented as a function of Pb+Pb collision centrality and distance from the jet axis for charged particles with transverse momenta in the 1−63 GeV range, matched to jets with transverse momenta in the 126−316 GeV range and an absolute value of jet rapidity of less than 1.7. Modifications to the measured distributions are quantified by taking a ratio to the measurements in pp collisions. Yields of charged particles with transverse momenta below 4 GeV are observed to be increasingly enhanced as a function of angular distance from the jet axis, reaching a maximum at r=0.6. Charged particles with transverse momenta above 4 GeV have an enhanced yield in Pb+Pb collisions in the jet core for angular distances up to r=0.05 from the jet axis, with a suppression at larger distances.
DOI: 10.17182/hepdata.91160.v1/t393
title: "Table 393" of "Measurement of angular and momentum distributions of charged particles within and around jets in Pb+Pb and $pp$ collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV with the ATLAS detector"

description: Figure 10. Delta_Theta The differences between charged particle distributions around jets as a function of distance from the jet axis integrated over 1-4 GeV charged particle pT in different centrality intervals of PbPb and pp collisions at 5.02 TeV for dfferent jet pT ranges.
description: CERN-LHC. Studies of the fragmentation of jets into charged particles in heavy-ion collisions can provide information about the mechanism of jet-quenching by the hot and dense QCD matter created in such collisions, the quark-gluon plasma. This paper presents a measurement of the angular distribution of charged particles around the jet axis in sNN=5.02 TeV Pb+Pb and pp collisions, using the ATLAS detector at the LHC. The Pb+Pb and pp data sets have integrated luminosities of 0.49 nb−1 and 25 pb−1, respectively. The measurement is performed for jets reconstructed with the anti-kt algorithm with radius parameter R=0.4 and is extended to an angular distance of r=0.8 from the jet axis. Results are presented as a function of Pb+Pb collision centrality and distance from the jet axis for charged particles with transverse momenta in the 1−63 GeV range, matched to jets with transverse momenta in the 126−316 GeV range and an absolute value of jet rapidity of less than 1.7. Modifications to the measured distributions are quantified by taking a ratio to the measurements in pp collisions. Yields of charged particles with transverse momenta below 4 GeV are observed to be increasingly enhanced as a function of angular distance from the jet axis, reaching a maximum at r=0.6. Charged particles with transverse momenta above 4 GeV have an enhanced yield in Pb+Pb collisions in the jet core for angular distances up to r=0.05 from the jet axis, with a suppression at larger distances.
DOI: 10.17182/hepdata.91160.v1/t394
title: "Table 394" of "Measurement of angular and momentum distributions of charged particles within and around jets in Pb+Pb and $pp$ collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV with the ATLAS detector"

description: Figure 11. R_Theta The ratios of charged particle distributions around jets as a function of distance from the jet axis integrated over 1-4 GeV charged particle pT in different centrality intervals of PbPb and pp collisions at 5.02 TeV for dfferent jet pT ranges.
description: CERN-LHC. Studies of the fragmentation of jets into charged particles in heavy-ion collisions can provide information about the mechanism of jet-quenching by the hot and dense QCD matter created in such collisions, the quark-gluon plasma. This paper presents a measurement of the angular distribution of charged particles around the jet axis in sNN=5.02 TeV Pb+Pb and pp collisions, using the ATLAS detector at the LHC. The Pb+Pb and pp data sets have integrated luminosities of 0.49 nb−1 and 25 pb−1, respectively. The measurement is performed for jets reconstructed with the anti-kt algorithm with radius parameter R=0.4 and is extended to an angular distance of r=0.8 from the jet axis. Results are presented as a function of Pb+Pb collision centrality and distance from the jet axis for charged particles with transverse momenta in the 1−63 GeV range, matched to jets with transverse momenta in the 126−316 GeV range and an absolute value of jet rapidity of less than 1.7. Modifications to the measured distributions are quantified by taking a ratio to the measurements in pp collisions. Yields of charged particles with transverse momenta below 4 GeV are observed to be increasingly enhanced as a function of angular distance from the jet axis, reaching a maximum at r=0.6. Charged particles with transverse momenta above 4 GeV have an enhanced yield in Pb+Pb collisions in the jet core for angular distances up to r=0.05 from the jet axis, with a suppression at larger distances.
DOI: 10.17182/hepdata.91160.v1/t395
title: "Table 395" of "Measurement of angular and momentum distributions of charged particles within and around jets in Pb+Pb and $pp$ collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV with the ATLAS detector"

description: Figure 11. R_P The ratios of charged particle distributions around jets as a function of cumulative distance from the jet axis integrated over 1-4 GeV charged particle pT in different centrality intervals of PbPb and pp collisions at 5.02 TeV for dfferent jet pT ranges.
description: CERN-LHC. Studies of the fragmentation of jets into charged particles in heavy-ion collisions can provide information about the mechanism of jet-quenching by the hot and dense QCD matter created in such collisions, the quark-gluon plasma. This paper presents a measurement of the angular distribution of charged particles around the jet axis in sNN=5.02 TeV Pb+Pb and pp collisions, using the ATLAS detector at the LHC. The Pb+Pb and pp data sets have integrated luminosities of 0.49 nb−1 and 25 pb−1, respectively. The measurement is performed for jets reconstructed with the anti-kt algorithm with radius parameter R=0.4 and is extended to an angular distance of r=0.8 from the jet axis. Results are presented as a function of Pb+Pb collision centrality and distance from the jet axis for charged particles with transverse momenta in the 1−63 GeV range, matched to jets with transverse momenta in the 126−316 GeV range and an absolute value of jet rapidity of less than 1.7. Modifications to the measured distributions are quantified by taking a ratio to the measurements in pp collisions. Yields of charged particles with transverse momenta below 4 GeV are observed to be increasingly enhanced as a function of angular distance from the jet axis, reaching a maximum at r=0.6. Charged particles with transverse momenta above 4 GeV have an enhanced yield in Pb+Pb collisions in the jet core for angular distances up to r=0.05 from the jet axis, with a suppression at larger distances.
DOI: 10.17182/hepdata.59488.v1/t11
title: "Table 11" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 40 TO 50%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t12
title: "Table 12" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 50 TO 60%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t4
title: "Table 4" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefficient V_n,n vs. |Delta(ETARAP)| for individual n values.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t5
title: "Table 5" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefficient V_n vs. |Delta(ETARAP)| from the 2PC anaysis for individual n values from 2 to n.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t6
title: "Table 6" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 0 TO 5%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t7
title: "Table 7" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 5 TO 10%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t8
title: "Table 8" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 10 TO 20%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t9
title: "Table 9" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 20 TO 30%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t10
title: "Table 10" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 30 TO 40%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t13
title: "Table 13" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 60 TO 70%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t14
title: "Table 14" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 0 TO 5%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t15
title: "Table 15" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 5 TO 10%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t16
title: "Table 16" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 10 TO 20%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.
DOI: 10.17182/hepdata.59488.v1/t17
title: "Table 17" of "Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector"

description: The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 20 TO 30%.
description: Differential measurements of charged particle azimuthal anisotropy are presented for lead-lead collisions at a centre-of-mass energy of 2.76 TeV/nucleon. The anisotropy is characterized via a Fourier expansion of the distribution of charged particles in azimuthal angle relative to the reaction plane, with the coefficients V_n denoting the magnitude of the anisotropy. A Fourier analysis of the charged particle pair distribution in relative angle is performed extracting the coefficients V_nn.