cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.105047.v1/t16
title: "Table 16" of "Measurement of beauty and charm production in pp collisions at $\sqrt{s}=5.02$ TeV via non-prompt and prompt D mesons"

description: $\mathrm{d}\sigma_\mathrm{b\overline{b}}/\mathrm{d} y$ estimated from non-prompt $\mathrm{{D^0}}$, $\mathrm{{D^+}}$ and $\mathrm{D_{s}^{+}}$ mesons (black circles of Figure 12) measured in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|&lt;0.5$. The average $\mathrm{d}\sigma_\mathrm{b\overline{b}}/\mathrm{d} y$ (red circle/diamond of Figure 12/13) of the estimates from the single D-meson species is also reported.
Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395
Branching ratio of $\mathrm{D^+\to K^-\pi^+\pi^+}$: 0.0938
Branching ratio of $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$: 0.0224
description: The $p_{\mathrm{T}}$-differential production cross sections of prompt and non-prompt (produced in beauty-hadron decays) D mesons were measured by the ALICE experiment at midrapidity ($|y|&lt;0.5$) in proton--proton collisions at $\sqrt{s}=5.02~\mathrm{TeV}$. The data sample used in the analysis corresponds to an integrated luminosity of $(19.3\pm0.4)~\mathrm{nb^{-1}}$. D mesons were reconstructed from their decays $\mathrm{D^0 \to K^-\pi^+}$, $\mathrm{D^+\to K^-\pi^+\pi^+}$, and $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$ and their charge conjugates. Compared to previous measurements in the same rapidity region, the cross sections of prompt $\mathrm{D^+}$ and $\mathrm{D_s^+}$ mesons have an extended $p_{\mathrm{T}}$ coverage and total uncertainties reduced by a factor ranging from 1.05 to 1.6, depending on $p_{\mathrm{T}}$, allowing for a more precise determination of their $p_{\mathrm{T}}$-integrated cross sections. The results are well described by perturbative QCD calculations. The fragmentation fraction of heavy quarks to strange mesons divided by the one to non-strange mesons, $f_\mathrm{s}/(f_\mathrm{u}+f_\mathrm{d})$, is compatible for charm and beauty quarks and with previous measurements at different centre-of-mass energies and collision systems. The $\mathrm{b\overline{b}}$ production cross section per rapidity unit at midrapidity, estimated from non-prompt D-meson measurements, is $\mathrm{d}\sigma_\mathrm{b\overline{b}}/\mathrm{d} y|_\mathrm{|y|&lt;0.5} = 34.5 \pm 2.4 (\mathrm{stat}) ^{+4.7}_{-2.9} (\mathrm{tot.~syst})~\mathrm{\mu b}$. It is compatible with previous measurements at the same centre-of-mass energy and with the cross section predicted by perturbative QCD calculations.
DOI: 10.17182/hepdata.105256.v1/t1
title: "Table 1" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_2${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 0-10% in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t2
title: "Table 2" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_2${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 30-50% in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t3
title: "Table 3" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_3${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 0-10% in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t5
title: "Table 5" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_2${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 0-10% and 20% small-$q_2$ sample, in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t6
title: "Table 6" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_2${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 0-10% and 20% large-$q_2$ sample, in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105047.v1/t17
title: "Table 17" of "Measurement of beauty and charm production in pp collisions at $\sqrt{s}=5.02$ TeV via non-prompt and prompt D mesons"

description: Production cross sections of prompt and non-prompt $\mathrm{{D^0}}$, $\mathrm{{D^+}}$ and $\mathrm{D_{s}^{+}}$ mesons in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|&lt;0.5$. The prompt $\mathrm{{D^0}}$ and $\mathrm{{D^+}}$ measurements are perfromed down to $p_\mathrm{{T}} = 0~\mathrm{GeV}/c$ and no extrapolation has been done (zero uncertainty assigned in the table).
Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395
Branching ratio of $\mathrm{D^+\to K^-\pi^+\pi^+}$: 0.0938
Branching ratio of $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$: 0.0224
description: The $p_{\mathrm{T}}$-differential production cross sections of prompt and non-prompt (produced in beauty-hadron decays) D mesons were measured by the ALICE experiment at midrapidity ($|y|&lt;0.5$) in proton--proton collisions at $\sqrt{s}=5.02~\mathrm{TeV}$. The data sample used in the analysis corresponds to an integrated luminosity of $(19.3\pm0.4)~\mathrm{nb^{-1}}$. D mesons were reconstructed from their decays $\mathrm{D^0 \to K^-\pi^+}$, $\mathrm{D^+\to K^-\pi^+\pi^+}$, and $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$ and their charge conjugates. Compared to previous measurements in the same rapidity region, the cross sections of prompt $\mathrm{D^+}$ and $\mathrm{D_s^+}$ mesons have an extended $p_{\mathrm{T}}$ coverage and total uncertainties reduced by a factor ranging from 1.05 to 1.6, depending on $p_{\mathrm{T}}$, allowing for a more precise determination of their $p_{\mathrm{T}}$-integrated cross sections. The results are well described by perturbative QCD calculations. The fragmentation fraction of heavy quarks to strange mesons divided by the one to non-strange mesons, $f_\mathrm{s}/(f_\mathrm{u}+f_\mathrm{d})$, is compatible for charm and beauty quarks and with previous measurements at different centre-of-mass energies and collision systems. The $\mathrm{b\overline{b}}$ production cross section per rapidity unit at midrapidity, estimated from non-prompt D-meson measurements, is $\mathrm{d}\sigma_\mathrm{b\overline{b}}/\mathrm{d} y|_\mathrm{|y|&lt;0.5} = 34.5 \pm 2.4 (\mathrm{stat}) ^{+4.7}_{-2.9} (\mathrm{tot.~syst})~\mathrm{\mu b}$. It is compatible with previous measurements at the same centre-of-mass energy and with the cross section predicted by perturbative QCD calculations.
DOI: 10.17182/hepdata.105256.v1/t4
title: "Table 4" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_3${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 30-50% in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t7
title: "Table 7" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_2${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 30-50% and 20% small-$q_2$ sample, in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t8
title: "Table 8" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Average $v_2${SP} vs. $p_\mathrm{T}$ of prompt D$^0$, D$^+$, and D$^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 30-50% and 20% large-$q_2$ sample, in the rapidity interval $|y|&lt;0.8$. The first (sys,data) error is the systematic uncertainty from all the other sources except for the B feed-down. The second (sys,FD) error is the systematic uncertainty from the B feed-down contribution.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t9
title: "Table 9" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Ratio of average prompt D$^0$, D$^+$, and D$^{*+}$ meson $v_2${SP} in the 20% small-$q_2$ sample and the unbiased sample vs. $p_\mathrm{T}$ in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 0-10% in the rapidity interval $|y|&lt;0.8$.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t11
title: "Table 11" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Ratio of average prompt D$^0$, D$^+$, and D$^{*+}$ meson $v_2${SP} in the 20% small-$q_2$ sample and the unbiased sample vs. $p_\mathrm{T}$ in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 30-50% in the rapidity interval $|y|&lt;0.8$.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t12
title: "Table 12" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Ratio of average prompt D$^0$, D$^+$, and D$^{*+}$ meson $v_2${SP} in the 20% large-$q_2$ sample and the unbiased sample vs. $p_\mathrm{T}$ in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 30-50% in the rapidity interval $|y|&lt;0.8$.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t13
title: "Table 13" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Ratio of average prompt D$^0$, D$^+$, and D$^{*+}$ meson $\mathrm{d}N/\mathrm{d}p_\mathrm{T}$ in the 20% small-$q_2$ sample and the unbiased sample vs. $p_\mathrm{T}$ in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 0-10% in the rapidity interval $|y|&lt;0.8$.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105256.v1/t10
title: "Table 10" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Ratio of average prompt D$^0$, D$^+$, and D$^{*+}$ meson $v_2${SP} in the 20% large-$q_2$ sample and the unbiased sample vs. $p_\mathrm{T}$ in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 0-10% in the rapidity interval $|y|&lt;0.8$.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105273.v1/t2
title: "Table 2" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: Results for the optimised observables FL and P1–P'8. The first uncertainties are statistical and the second systematic.
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105273.v1/t3
title: "Fig 3a" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: The CP-averaged observable Fl versus q2. The first (second) error bars represent the statistical (total) uncertainties.
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105273.v1/t4
title: "Fig 3b" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: The CP-averaged observable S3 versus q2. The first (second) error bars represent the statistical (total) uncertainties.
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.
DOI: 10.17182/hepdata.105256.v1/t15
title: "Table 15" of "Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV"

description: Ratio of average prompt D$^0$, D$^+$, and D$^{*+}$ meson $\mathrm{d}N/\mathrm{d}p_\mathrm{T}$ in the 20% small-$q_2$ sample and the unbiased sample vs. $p_\mathrm{T}$ in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV in the centrality class 30-50% in the rapidity interval $|y|&lt;0.8$.
description: CERN LHC. The elliptic and triangular flow coefficients $v_2$ and $v_3$ of prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\mathrm{D}^{*+}$ mesons were measured at mid rapidity ($|y|&lt;0.8$) in Pb-Pb collisions at the centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays in the transverse momentum interval $1
DOI: 10.17182/hepdata.105273.v1/t7
title: "Fig 3e" of "Angular analysis of the $B^{+}\rightarrow K^{\ast+}\mu^{+}\mu^{-}$ decay"

description: The CP-averaged observable Afb versus q2. The first (second) error bars represent the statistical (total) uncertainties.
description: CERN-LHC. Measurements of the angular observables in the B+ --&gt; K*+ mu+ mu- decay with K*+ --&gt; KS0 pi+ and KS0 -&gt; pi+ pi- using proton-proton collisions at a centre-of-mass energy of 7, 8 and 13 TeV with 9 fb^-1 of data collected in 2011-2018. The final states used are 3 charged pions and 2 muons. The fit is performed simultaneously in the sub sets of Run 1 and 2 and the two distinct KS0 categories, whether or not the KS0 decays inside the Vertex Locator or not. Values for the observables in two angular basis are determined, namely the S and P(') basis.

The reported central values of the angular observables in Table 1 and 2 are evaluated using angular folding techniques. The asymmetric statistical uncertainties are obtained by Feldman-Cousins scans. The correlation between all observables are determined using a bootstrapping method.