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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV ; volume:2022 ; number:12 ; day:21 ; month:12 ; year:2022 ; pages:1-28 ; date:12.2022
Journal of high energy physics ; 2022, Heft 12 (21.12.2022), 1-28, 12.2022

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP12(2022)126

URN: urn:nbn:de:101:1-2023030621072718040664

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

Last update: 14.08.2025, 10:55 AM CEST

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Other Objects (12)

$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

$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

$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

$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$

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

$Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 5.02 TeV$

Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 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

$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

$Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV$

Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV

$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

$Measurement of inclusive and leading subjet fragmentation in pp and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of inclusive and leading subjet fragmentation in pp and 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$

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

$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

$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

$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$

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

$Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 5.02 TeV$

Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 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

$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

$Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV$

Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV

$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

$Measurement of inclusive and leading subjet fragmentation in pp and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of inclusive and leading subjet fragmentation in pp and 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$

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

$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

$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

$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$

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

$Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 5.02 TeV$

Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 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

$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

$Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV$

Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV

$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

$Measurement of inclusive and leading subjet fragmentation in pp and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of inclusive and leading subjet fragmentation in pp and 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$

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

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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

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Other Objects (12)

Azimuthal anisotropy of jet particles in p-Pb and 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

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

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

Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 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

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

Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV

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

Measurement of inclusive and leading subjet fragmentation in pp and 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

Azimuthal anisotropy of jet particles in p-Pb and 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

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

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

Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 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

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

Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV

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

Measurement of inclusive and leading subjet fragmentation in pp and 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

Azimuthal anisotropy of jet particles in p-Pb and 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

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

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

Dielectron production at midrapidity at low transverse momentum in peripheral and semi-peripheral Pb–Pb collisions at s NN $$ \sqrt{s}}_{\textrm{NN}} $$ = 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

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

Particle production in a hybrid approach for a beam energy scan of Au+Au/Pb+Pb collisions between $$\sqrts_\textrm{NN}}$$ s NN = 4.3 GeV and $$\sqrts_\textrm{NN}}$$ s NN = 200.0 GeV

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

Measurement of inclusive and leading subjet fragmentation in pp and 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

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