cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.127978.v1/t15
title: "Table 15" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in pp collisions at $\sqrt{s}$ = 13 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t16
title: "Table 16" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\rm{K}^{0}_{S}$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t17
title: "Table 17" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t18
title: "Table 18" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\phi$ meson measured in pp collisions at $\sqrt{s}$ = 13 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t19
title: "Table 19" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Random Plane for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t21
title: "Table 21" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 0.4-1.2 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t22
title: "Table 22" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t23
title: "Table 23" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 0.5-0.8 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t28
title: "Table 28" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t20
title: "Table 20" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Random Plane for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t24
title: "Table 24" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t25
title: "Table 25" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 0.8-1.2 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127978.v1/t27
title: "Table 27" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 0.5-0.7 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127979.v1/t1
title: "Table 1" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse momentum distributions d$N$/(d$y$d$p_{\mathrm{T}}$) of prompt D$^{0}$ (left) meson in the 0-10% (crosses) centrality classes in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in |y|&lt;0.5. The uncertainties on the BRs are quoted separately and the horizontal bars represent bin widths. Branching ratio of D$^0$ --&gt; K$\pi$ = 0.0395
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
DOI: 10.25549/vercoutere-ouc110611605
title: Toreros

description: Six men dressed in black pants, black capes, gray knee-high boots, flat black hats with red trim carrying swords or lances; three shorter men (or women) dressed in black pants, gray or turquoise boots, with red capes (two covering their heads and one covered from shoulders is wearing a red hat) Background is green, cream, and brown.
DOI: 10.17182/hepdata.127978.v1/t26
title: "Table 26" of "Measurement of spin-orbital angular momentum interactions in relativistic heavy-ion collisions"

description: $\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.127979.v1/t4
title: "Table 4" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse momentum distributions d$N$/(d$y$d$p_{\mathrm{T}}$) of prompt D$^{+}$ (middle) meson in the 30-50% (diamonds) centrality classes in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in |y|&lt;0.5. The uncertainties on the BRs are quoted separately and the horizontal bars represent bin widths. The points in the figure of the paper are scaled for visibility by a factor 10$^{-1}$. Branching ratio of D$^+$ --&gt; K$\pi\pi$ = 0.0938
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
DOI: 10.17182/hepdata.127979.v1/t5
title: "Table 5" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse momentum distributions d$N$/(d$y$d$p_{\mathrm{T}}$) of prompt D*$^{+}$ (right) meson in the 0-10% (crosses) centrality classes in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in |y|&lt;0.5. The uncertainties on the BRs are quoted separately and the horizontal bars represent bin widths. Branching ratio of D*$^+$ --&gt; D$^0\pi$ = 0.677
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
DOI: 10.17182/hepdata.127979.v1/t6
title: "Table 6" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse momentum distributions d$N$/(d$y$d$p_{\mathrm{T}}$) of prompt D*$^{+}$ (right) meson in the 30-50% (diamonds) centrality classes in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in |y|&lt;0.5. The uncertainties on the BRs are quoted separately and the horizontal bars represent bin widths. The points in the figure of the paper are scaled for visibility by a factor 10$^{-1}$. Branching ratio of D*$^+$ --&gt; D$^0\pi$ = 0.677
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
DOI: 10.17182/hepdata.127979.v1/t7
title: "Table 7" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Ratio D$^{+}$/D$^{0}$ in central Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in |y|&lt;0.5 and as a function of $p_\mathrm{T}$. Statistical (bars) and systematic (boxes) uncertainties are shown. Branching ratio of D$^0$ --&gt; K$\pi$ = 0.0395 Branching ratio of D$^+$ --&gt; K$\pi\pi$ = 0.0938
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
DOI: 10.17182/hepdata.127979.v1/t8
title: "Table 8" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Ratio D$^{+}$/D$^{0}$ in semicentral Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in |y|&lt;0.5 and as a function of $p_\mathrm{T}$. Statistical (bars) and systematic (boxes) uncertainties are shown. Branching ratio of D$^0$ --&gt; K$\pi$ = 0.0395 Branching ratio of D$^+$ --&gt; K$\pi\pi$ = 0.0938
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
DOI: 10.17182/hepdata.127979.v1/t9
title: "Table 9" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Ratio D*$^{+}$/D$^{0}$ in central Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in |y|&lt;0.5 and as a function of $p_\mathrm{T}$. Statistical (bars) and systematic (boxes) uncertainties are shown. Branching ratio of D$^0$ --&gt; K$\pi$ = 0.0395 Branching ratio of D*$^+$ --&gt; D$^0\pi$ = 0.677
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.
DOI: 10.17182/hepdata.127979.v1/t10
title: "Table 10" of "Prompt D$^{0}$, D$^{+}$, and D$^{*+}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Ratio D*$^{+}$/D$^{0}$ in semicentral Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in |y|&lt;0.5 and as a function of $p_\mathrm{T}$. Statistical (bars) and systematic (boxes) uncertainties are shown. Branching ratio of D$^0$ --&gt; K$\pi$ = 0.0395 Branching ratio of D*$^+$ --&gt; D$^0\pi$ = 0.677
description: CERN LHC. The production of prompt D$^{0}$, D$^{+}$, and D*$^{+}$ mesons was measured at midrapidity ($|y|&lt;0.5$) in Pb-Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decay channels and their production yields were measured in central (0-10%) and semicentral (30-50%) collisions. The measurement was performed up to a transverse momentum ($p_\mathrm{T}$) of 36 or 50 GeV/$c$ depending on the D meson species and the centrality interval. For the first time in Pb-Pb collisions at the LHC, the yield of D$^{0}$ mesons was measured down to $p_\mathrm{T} =$ 0, which allowed a model-independent determination of the $p_\mathrm{T}$-integrated yield per unit of rapidity (d$N$/d$y$). A maximum suppression by a factor 5 and 2.5 was observed with the nuclear modification factor ($R_{\mathrm{AA}}$) of prompt D mesons at $p_\mathrm{T} =$ 6-8 GeV/$c$ for the 0-10% and 30-50% centrality classes, respectively. The D-meson $R_{\mathrm{AA}}$ is compared with that of charged pions, charged hadrons, and J/$\psi$ mesons as well as with theoretical predictions. The analysis of the agreement between the measured $R_{\mathrm{AA}}$, elliptic ($v_{2}$) and triangular ($v_{3}$) flow, and the model predictions allowed us to constrain the charm spatial diffusion coefficient $D_{s}$. Furthermore the comparison of $R_{\mathrm{AA}}$ and $v_{2}$ with different implementations of the same models provides an important insight into the role of radiative energy loss as well as charm quark recombination in the hadronisation mechanisms.