Search results for "PbPb"

showing 10 items of 82 documents

"Table 2" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

2020

Second cumulants of the Skellam distribution.

1276.0PbPbkappa2(Skellam)
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"Table 6" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

2020

Measured first cumulants of anti-protons.

1276.0kappa1(barp)PbPb
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"Table 9" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

2020

R2 values from Model.

Model R21276.0PbPb
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"Table 88" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2019

Excess transverse momenta in jet in PbPb compared to pp collisions in different centrality selections for abs(jet rapidity) < 2.1.

PB PB --> JETS X5020.0PbPb) - D(pTAstrophysics::High Energy Astrophysical Phenomenapp)High Energy Physics::ExperimentpT < 4 GeVNuclear Experimentp p --> JETS XNch = D(pTjet fragmentation functions
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"Table 84" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

Excess transverse momenta in jet in PbPb compared to pp collisions in different centrality selections for abs(jet rapidity) < 2.1.

PB PB --> JETS X5020.0PbPb) - D(pTAstrophysics::High Energy Astrophysical Phenomenapp)High Energy Physics::ExperimentpT < 4 GeVNuclear Experimentp p --> JETS XNch = D(pTjet fragmentation functions
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"Table 85" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

Excess particles in jet in PbPb compared to pp collisions in different centrality selections for abs(jet rapidity) < 2.1.

PB PB --> JETS X5020.0PbPb) - D(pTpp)) * pTpTch = (D(pTpT < 4 GeVp p --> JETS Xjet fragmentation functions
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"Table 89" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2019

Excess particles in jet in PbPb compared to pp collisions in different centrality selections for abs(jet rapidity) < 2.1.

PB PB --> JETS X5020.0PbPb) - D(pTpp)) * pTpTch = (D(pTpT < 4 GeVp p --> JETS Xjet fragmentation functions
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"Table 63" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2019

The ratio of the D(pT) in different centrality intervals in PbPb and in pp for 199.53 < pTjet < 251.19 and 0.8 < eta < 1.2.

PB PB --> JETS XD(pT5020.0pp)PbPb) / D(pTp p --> JETS Xjet fragmentation functions
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"Table 75" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2019

The ratio of the D(pT) in different centrality intervals in PbPb and in pp for 251.19 < pTjet < 316.22 and 0.3 < eta < 0.8.

PB PB --> JETS XD(pT5020.0pp)PbPb) / D(pTp p --> JETS Xjet fragmentation functions
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"Table 87" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2019

The ratio of the D(pT) in different centrality intervals in PbPb and in pp for 251.19 < pTjet < 316.22 and 0.0 < eta < 2.1.

PB PB --> JETS XD(pT5020.0pp)PbPb) / D(pTp p --> JETS Xjet fragmentation functions
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