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D-meson RAA in Pb-Pb collisions at 5.02 TeV - 2018 data sample

$\mathrm{D}^0$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 1.5 < $p_{\mathrm{T}}$ < 2 GeV/$c$ (0-10% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_D0_PbPb2018_5TeV_pt_1.5_2.0_010.eps
Figure image (.pdf)
2019-10-31-InvMass_D0_PbPb2018_5TeV_pt_1.5_2.0_010.pdf
$\mathrm{D}^0$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 1.5 < $p_{\mathrm{T}}$ < 2 GeV/$c$ (30-50% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_D0_PbPb2018_5TeV_pt_1.5_2.0_3050.eps
Figure image (.pdf)
2019-10-31-InvMass_D0_PbPb2018_5TeV_pt_1.5_2.0_3050.pdf
$\mathrm{D}^+$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 5 < $p_{\mathrm{T}}$ < 5.5 GeV/$c$ (0-10% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_Dplus_PbPb2018_5TeV_pt_5.0_5.5_010.eps
Figure image (.pdf)
2019-10-31-InvMass_Dplus_PbPb2018_5TeV_pt_5.0_5.5_010.pdf
$\mathrm{D}^+$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 16 < $p_{\mathrm{T}}$ < 24 GeV/$c$ (30-50% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_Dplus_PbPb2018_5TeV_pt_16.0_24.0_3050.eps
Figure image (.pdf)
2019-10-31-InvMass_Dplus_PbPb2018_5TeV_pt_16.0_24.0_3050.pdf
$\mathrm{D}^{*+}$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 16 < $p_{\mathrm{T}}$ < 24 GeV/$c$ (0-10% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_Dstar_PbPb2018_5TeV_pt_16.0_24.0_010.eps
Figure image (.pdf)
2019-10-31-InvMass_Dstar_PbPb2018_5TeV_pt_16.0_24.0_010.pdf
$\mathrm{D}^{*+}$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 7.5 < $p_{\mathrm{T}}$ < 8 GeV/$c$ (30-50% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_Dstar_PbPb2018_5TeV_pt_7.5_8.0_3050.eps
Figure image (.pdf)
2019-10-31-InvMass_Dstar_PbPb2018_5TeV_pt_7.5_8.0_3050.pdf
$\mathrm{D}_{s}$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 3 < $p_{\mathrm{T}}$ < 4 GeV/$c$ (0-10% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_Ds_PbPb2018_5TeV_pt_3.0_4.0_010.eps
Figure image (.pdf)
2019-10-31-InvMass_Ds_PbPb2018_5TeV_pt_3.0_4.0_010.pdf
$\mathrm{D}_{s}$ invariant mass distribution in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in the interval 3 < $p_{\mathrm{T}}$ < 4 GeV/$c$ (30-50% central)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMass_Ds_PbPb2018_5TeV_pt_3.0_4.0_3050.eps
Figure image (.pdf)
2019-10-31-InvMass_Ds_PbPb2018_5TeV_pt_3.0_4.0_3050.pdf
Efficiency $\times$ acceptance for $\mathrm{D}^0$ in 0-10% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DzeroAccEffVsPt_PbPb_5TeV_010.eps
Figure image (.pdf)
2019-10-31-DzeroAccEffVsPt_PbPb_5TeV_010.pdf
Efficiency $\times$ acceptance for $\mathrm{D}^0$ in 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DzeroAccEffVsPt_PbPb_5TeV_3050.eps
Figure image (.pdf)
2019-10-31-DzeroAccEffVsPt_PbPb_5TeV_3050.pdf
Efficiency $\times$ acceptance for $\mathrm{D}^+$ in 0-10% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DplusAccEffVsPt_PbPb_5TeV_010.eps
Figure image (.pdf)
2019-10-31-DplusAccEffVsPt_PbPb_5TeV_010.pdf
Efficiency $\times$ acceptance for $\mathrm{D}^+$ in 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DplusAccEffVsPt_PbPb_5TeV_3050.eps
Figure image (.pdf)
2019-10-31-DplusAccEffVsPt_PbPb_5TeV_3050.pdf
Efficiency $\times$ acceptance for $\mathrm{D}^{*+}$ in 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DstarAccEffVsPt_PbPb_5TeV_3050.eps
Figure image (.pdf)
2019-10-31-DstarAccEffVsPt_PbPb_5TeV_3050.pdf
Efficiency $\times$ acceptance for $\mathrm{D}_{s}$ in 0-10% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DsAccEffVsPt_PbPb_5TeV_010.eps
Figure image (.pdf)
2019-10-31-DsAccEffVsPt_PbPb_5TeV_010.pdf
Efficiency $\times$ acceptance for $\mathrm{D}_{s}$ in 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DsAccEffVsPt_PbPb_5TeV_3050.eps
Figure image (.pdf)
2019-10-31-DsAccEffVsPt_PbPb_5TeV_3050.pdf
Efficiency $\times$ acceptance for $\mathrm{D}^{*+}$ in 0-10% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DstarAccEffVsPt_PbPb_5TeV_010.eps
Figure image (.pdf)
2019-10-31-DstarAccEffVsPt_PbPb_5TeV_010_0.pdf
$\mathrm{D}^0$ corrected $p_{\mathrm{T}}$-spectra in 0-10% and 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Dzero_dNdpt_010_3050.eps
Figure image (.pdf)
2019-10-31-Dzero_dNdpt_010_3050.pdf
$\mathrm{D}^+$ corrected $p_{\mathrm{T}}$-spectra in 0-10% and 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Dplus_dNdpt_010_3050.eps
Figure image (.pdf)
2019-10-31-Dplus_dNdpt_010_3050.pdf
$\mathrm{D}^{*+}$ corrected $p_{\mathrm{T}}$-spectra in 0-10% and 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Dstar_dNdpt_010_3050.eps
Figure image (.pdf)
2019-10-31-Dstar_dNdpt_010_3050.pdf
$\mathrm{D}_{s}$ corrected $p_{\mathrm{T}}$-spectra in 0-10% and 30-50% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Ds_dNdpt_010_3050.eps
Figure image (.pdf)
2019-10-31-Ds_dNdpt_010_3050.pdf
$\mathrm{D}^0$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10%, 30-50% and 60-80%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Dzero_010_3050_6080_comparison_.eps
Figure image (.pdf)
2019-10-31-Dzero_010_3050_6080_comparison_.pdf
Non-strange D-meson average $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10%, 30-50% and 60-80%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_010_3050_6080_comparison_.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_010_3050_6080_comparison_.pdf
Non-strange D-meson average $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_010.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_010.pdf
Non-strange D-meson average $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_3050.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_3050.pdf
Non-strange D-meson average $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10% (2018 vs 2015)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DaverageRAA_5TeV_010_2018_2015.eps
Figure image (.pdf)
2019-10-31-DaverageRAA_5TeV_010_2018_2015.pdf
Non-strange D-meson average $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50% (2018 vs 2015)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DaverageRAA_5TeV_3050_2018_2015.eps
Figure image (.pdf)
2019-10-31-DaverageRAA_5TeV_3050_2018_2015.pdf
Comparison of $\mathrm{D}^0$, $\mathrm{D}^+$ and $\mathrm{D}^{*+}$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonComparison_010.eps
Figure image (.pdf)
2019-10-31-DmesonComparison_010.pdf
Charged particles, pions and average prompt non-strange D-meson $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DPionRaaAnd5TeV_010_2018.eps
Figure image (.pdf)
2019-10-31-DPionRaaAnd5TeV_010_2018.pdf
Charged particles, pions and average prompt non-strange D-meson $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DPionRaaAnd5TeV_3050_2018.eps
Figure image (.pdf)
2019-10-31-DPionRaaAnd5TeV_3050_2018.pdf
Prompt non-strange D and $\mathrm{D}_{s}$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverageDs_010.eps
Figure image (.pdf)
2019-10-31-DmesonAverageDs_010.pdf
Prompt non-strange D and $\mathrm{D}_{s}$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverageDs_3050.eps
Figure image (.pdf)
2019-10-31-DmesonAverageDs_3050.pdf
Prompt non-strange D and $\mathrm{D}_{s}$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50% with transport models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverageDs_vs_models_3050_5dot02.eps
Figure image (.pdf)
2019-10-31-DmesonAverageDs_vs_models_3050_5dot02.pdf
Prompt non-strange D mesons $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10% with transport models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_vs_transportmodels_010_5dot02.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_vs_transportmodels_010_5dot02.pdf
Prompt non-strange D mesons $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50% with transport models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_vs_transportmodels_3050_5dot02.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_vs_transportmodels_3050_5dot02.pdf
Prompt non-strange D mesons $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10% with pQCD models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_vs_pQCDmodels_010_5dot02.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_vs_pQCDmodels_010_5dot02.pdf
Prompt non-strange D mesons $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50% with pQCD models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_vs_pQCDmodels_3050_5dot02_band.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_vs_pQCDmodels_3050_5dot02_band.pdf
Prompt non-strange D mesons $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50% with pQCD models (high $p_{\mathrm{T}}$ highlight)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_vs_pQCDmodels_logY_3050_5dot02.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_vs_pQCDmodels_logY_3050_5dot02.pdf
$\mathrm{D}^+$/$\mathrm{D}^0$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV (2018 data sample)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Dplus_over_D0_PbPb2018_010_3050.eps
Figure image (.pdf)
2019-10-31-Dplus_over_D0_PbPb2018_010_3050.pdf
$\mathrm{D}^{*+}$/$\mathrm{D}^0$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV (2018 data sample)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Dstar_over_D0_PbPb2018_010_3050.eps
Figure image (.pdf)
2019-10-31-Dstar_over_D0_PbPb2018_010_3050.pdf
$\mathrm{D}_{s}$/$\mathrm{D}^0$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV (2018 data sample)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Ds_over_D0_PbPb2018_010_3050.eps
Figure image (.pdf)
2019-10-31-Ds_over_D0_PbPb2018_010_3050.pdf
Double-ratio of $\mathrm{D}^+$/$\mathrm{D}^0$ in Pb-Pb and in pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DoubleRatio_Dplus_over_D0_PbPb2018_010_3050_pp.eps
Figure image (.pdf)
2019-10-31-DoubleRatio_Dplus_over_D0_PbPb2018_010_3050_pp.pdf
Double-ratio of $\mathrm{D}^{*+}$/$\mathrm{D}^0$ in Pb-Pb and in pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DoubleRatio_Dstar_over_D0_PbPb2018_010_3050_pp.eps
Figure image (.pdf)
2019-10-31-DoubleRatio_Dstar_over_D0_PbPb2018_010_3050_pp.pdf
Double-ratio of $\mathrm{D}_{s}$/$\mathrm{D}^0$ in Pb-Pb and in pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DoubleRatio_Ds_over_D0_PbPb2018_010_3050_pp.eps
Figure image (.pdf)
2019-10-31-DoubleRatio_Ds_over_D0_PbPb2018_010_3050_pp.pdf
Double-ratio of $\mathrm{D}_{s}$/$\mathrm{D}^+$ in Pb-Pb and in pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DoubleRatio_Ds_over_Dplus_PbPb2018_010_3050_pp.eps
Figure image (.pdf)
2019-10-31-DoubleRatio_Ds_over_Dplus_PbPb2018_010_3050_pp.pdf
Double-ratio of $\mathrm{D}_{s}$/$\mathrm{D}^0$ in 0-10% Pb-Pb and in pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV with transport models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DoubleRatio_DsOverDzero_PbPb2018_010_pp_WithModels.eps
Figure image (.pdf)
2019-10-31-DoubleRatio_DsOverDzero_PbPb2018_010_pp_WithModels.pdf
Double-ratio of $\mathrm{D}_{s}$/$\mathrm{D}^0$ in 30-50% Pb-Pb and in pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV with transport models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2020-02-17-DoubleRatio_DsOverDzero_PbPb2018_3050_pp_WithModels.eps
Figure image (.pdf)
2020-02-17-DoubleRatio_DsOverDzero_PbPb2018_3050_pp_WithModels.pdf
Double-ratio of $\mathrm{D}_{s}$/$\mathrm{D}^0$ in Pb-Pb and in pp collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV with transport models (three panels)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2020-02-17-DoubleRatio_DsOverDzero_PbPb2018_010_3050_pp_WithModels.eps
Figure image (.pdf)
2020-02-17-DoubleRatio_DsOverDzero_PbPb2018_010_3050_pp_WithModels.pdf
$\mathrm{D}_{s}$/$\mathrm{D}^+$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV (2018 data sample)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Ds_over_Dplus_PbPb2018_010_3050.eps
Figure image (.pdf)
2019-10-31-Ds_over_Dplus_PbPb2018_010_3050.pdf
Prompt non-strange D and $\mathrm{D}_{s}$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10% with transport models
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverageDs_vs_models_010_5dot02.eps
Figure image (.pdf)
2019-10-31-DmesonAverageDs_vs_models_010_5dot02.pdf
Prompt non-strange D mesons $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10% with pQCD models (high $p_{\mathrm{T}}$ highlight)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_vs_pQCDmodels_logY_010_5dot02.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_vs_pQCDmodels_logY_010_5dot02.pdf
Average non-strange D-meson $R_{\mathrm{AA}}$ (ALICE) and prompt $\mathrm{D}^{0}$ (CMS) in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverageCMS_010_2018.eps
Figure image (.pdf)
2019-10-31-DmesonAverageCMS_010_2018.pdf
Comparison of $\mathrm{D}^0$, $\mathrm{D}^+$ and $\mathrm{D}^{*+}$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 30-50%
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonComparison_3050.eps
Figure image (.pdf)
2019-10-31-DmesonComparison_3050.pdf
Efficiency $\times$ acceptance for $\mathrm{D}^{*+}$ in 0-10% central Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DstarAccEffVsPt_PbPb_5TeV_010.eps
Figure image (.pdf)
2019-10-31-DstarAccEffVsPt_PbPb_5TeV_010.pdf
D0 candidate invariant mass distribution in 0<pt<1 GeV/c for Pb-Pb (low-pt analysis)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-InvMassSpectraEvMix_LowPtD0_PbPb010_bin0.eps
Figure image (.pdf)
2019-10-31-InvMassSpectraEvMix_LowPtD0_PbPb010_bin0.pdf
D0 yield in Pb-Pb collisions (0-10% centrality) from low-pt analysis compared to pp reference
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-Dzero-dNdpt-010PbPb.eps
Figure image (.pdf)
2019-10-31-Dzero-dNdpt-010PbPb.pdf
D0 RAA in Pb-Pb collisions (0-10% centrality) from low-pt analysis compared to analysis with topological cuts
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-RAA-LowPt_Topol.eps
Figure image (.pdf)
2019-10-31-RAA-LowPt_Topol.pdf
D0 pt-integrated nuclear modification factor in 0-10% Pb-Pb collisions and 0-100% p-Pb collisions
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2020-02-23-Dzero-RAA-PtIntegr-withyrange.eps
Figure image (.pdf)
2020-02-23-Dzero-RAA-PtIntegr-withyrange.pdf
Prompt non-strange D and $\mathrm{D}_{s}$ $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10% with transport models (linear x-scale)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverageDs_vs_models_010_5dot02_linX.eps
Figure image (.pdf)
2019-10-31-DmesonAverageDs_vs_models_010_5dot02_linX.pdf
Prompt non-strange D mesons $R_{\mathrm{AA}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in 0-10% with transport models (linear x-scale)
Energy
5.02 TeV
System
Pb-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
2019-10-31-DmesonAverage_vs_transportmodels_010_5dot02_linX.eps
Figure image (.pdf)
2019-10-31-DmesonAverage_vs_transportmodels_010_5dot02_linX.pdf