Measurement of D0, D+, D*+ and D s + production in Pb-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV

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Alternative title: 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Measurement of D0, D+, D*+ and D s + production in Pb-Pb collisions at s N N ; volume:2018 ; number:10 ; day:29 ; month:10 ; year:2018 ; pages:1-35 ; date:10.2018
Journal of high energy physics ; 2018, Heft 10 (29.10.2018), 1-35, 10.2018

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2018)174

URN: urn:nbn:de:101:1-2018122023412926159867

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

Last update: 14.08.2025, 10:47 AM CEST

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Other Objects (12)

$Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV$

Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV

$Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV$

Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV

$Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV$

Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

$Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV$

Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV

$Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV$

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

$Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]$

Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]

$Measurement of $${\mathrm{D}}^0}$$ D0 , $${\mathrm{D}}^+}$$ D+ , $${\mathrm{D}}^{*+}}$$ D∗+ and $${\mathrm{D}}^+_{\mathrm{s}}}$$ Ds+ production in pp collisions at $$\sqrt{{\textit{s}}}~=~5.02~{\text TeV}}}$$ s=5.02TeV with ALICE$

Measurement of $${\mathrm{D}}^0}$$ D0 , $${\mathrm{D}}^+}$$ D+ , $${\mathrm{D}}^{*+}}$$ D∗+ and $${\mathrm{D}}^+_{\mathrm{s}}}$$ Ds+ production in pp collisions at $$\sqrt{{\textit{s}}}~=~5.02~{\text TeV}}}$$ s=5.02TeV with ALICE

$Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}$

Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}

$Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV$

Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV

$Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]$

Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]

$Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions$

Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions

$Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV$

Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV

$Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV$

Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV

$Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV$

Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

$Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV$

Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV

$Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV$

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

$Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]$

Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]

Measurement of $${\mathrm{D}}^0}$$ D0 , $${\mathrm{D}}^+}$$ D+ , $${\mathrm{D}}^{*+}}$$ D∗+ and $${\mathrm{D}}^+_{\mathrm{s}}}$$ Ds+ production in pp collisions at $$\sqrt{{\textit{s}}}~=~5.02~{\text TeV}}}$$ s=5.02TeV with ALICE

$Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}$

Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}

$Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV$

Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV

$Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]$

Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]

$Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions$

Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions

$Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV$

Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV

$Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV$

Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV

$Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV$

Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

$Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV$

Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV

$Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV$

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

$Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]$

Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]

Measurement of $${\mathrm{D}}^0}$$ D0 , $${\mathrm{D}}^+}$$ D+ , $${\mathrm{D}}^{*+}}$$ D∗+ and $${\mathrm{D}}^+_{\mathrm{s}}}$$ Ds+ production in pp collisions at $$\sqrt{{\textit{s}}}~=~5.02~{\text TeV}}}$$ s=5.02TeV with ALICE

$Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}$

Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}

$Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV$

Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV

$Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]$

Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]

$Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions$

Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions

$Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

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Measurement of D0, D+, D*+ and D s + production in Pb-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV

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Other Objects (12)

Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV

Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV

Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]

Measurement of $${\mathrm{D}}^0}$$ D0 , $${\mathrm{D}}^+}$$ D+ , $${\mathrm{D}}^{*+}}$$ D∗+ and $${\mathrm{D}}^+_{\mathrm{s}}}$$ Ds+ production in pp collisions at $$\sqrt{{\textit{s}}}~=~5.02~{\text TeV}}}$$ s=5.02TeV with ALICE

Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}

Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV

Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]

Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV

Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV

Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]

Measurement of $${\mathrm{D}}^0}$$ D0 , $${\mathrm{D}}^+}$$ D+ , $${\mathrm{D}}^{*+}}$$ D∗+ and $${\mathrm{D}}^+_{\mathrm{s}}}$$ Ds+ production in pp collisions at $$\sqrt{{\textit{s}}}~=~5.02~{\text TeV}}}$$ s=5.02TeV with ALICE

Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}

Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV

Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]

Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Measurement of prompt D0, D+, D*+, and D S + $$ \mathrm{D}}_{\mathrm{S}}^{+} $$ production in p–Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ : = 5.02 TeV

Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV

Jet properties in PbPb and pp collisions at sNN=5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

Coherent photoproduction of ρ 0 vector mesons in ultra-peripheral Pb-Pb collisions at s NN $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}} $$ = 5.02 TeV

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

Measurement of D-meson production versus multiplicity in p-Pb collisions at s N N : = 5.02 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=5.02 $$ TeV [[electronic resource]]

Measurement of $${\mathrm{D}}^0}$$ D0 , $${\mathrm{D}}^+}$$ D+ , $${\mathrm{D}}^{*+}}$$ D∗+ and $${\mathrm{D}}^+_{\mathrm{s}}}$$ Ds+ production in pp collisions at $$\sqrt{{\textit{s}}}~=~5.02~{\text TeV}}}$$ s=5.02TeV with ALICE

Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV}

Coherent $$\mathrmJ}/\psi $$ J / ψ and $$\uppsi '}$$ ψ ′ photoproduction at midrapidity in ultra-peripheral Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}~=~5.02$$ s NN = 5.02 TeV

Centrality dependence of ψ(2S) suppression in p-Pb collisions at s N N : = 5.02 $$ \sqrt{s}}_{\mathrm{NN}}=5.02 $$ TeV [[electronic resource]]

Jet fragmentation transverse momentum measurements from di-hadron correlations in s : = 7 $$ \sqrt\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

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