Measurement of non-prompt $${\textrm{D}}^{0}}$$ D 0 -meson elliptic flow in Pb–Pb collisions at $$\sqrts_{\textrm{NN}}} = 5.02$$ s NN = 5.02 TeV

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: Measurement of non-prompt $${\textrm{D}}^{0}}$$ D 0 -meson elliptic flow in Pb–Pb collisions at $$\sqrts_{\textrm{NN}}} = 5.02$$ s NN = 5.02 TeV ; volume:83 ; number:12 ; day:11 ; month:12 ; year:2023 ; pages:1-17 ; date:12.2023
The European physical journal / C. C, Particles and fields ; 83, Heft 12 (11.12.2023), 1-17, 12.2023

Contributor: SpringerLink (Online service)

DOI: 10.1140/epjc/s10052-023-12259-3

URN: urn:nbn:de:101:1-2405271052409.793851681458

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:50 AM CEST

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$Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV$

Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV

$Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV$

Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV

$Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV$

Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV

$Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

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Measurement of non-prompt $${\textrm{D}}^{0}}$$ D 0 -meson elliptic flow in Pb–Pb collisions at $$\sqrts_{\textrm{NN}}} = 5.02$$ s NN = 5.02 TeV

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Other Objects (12)

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV

Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV

Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Prompt and non-prompt J/ψ production at midrapidity in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Energy dependence of coherent photonuclear production of J/ψ mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Transverse momentum decorrelation of the flow vector in Pb–Pb collisions at $$\sqrts_{_{\textrm{NN}}}}$$ s NN = 5.02 TeV

Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

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