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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $ \sqrt{{s_{\mathrm{NN}}}}}=2.76\;\mathrm{TeV} ; volume:2012 ; number:9 ; day:25 ; month:9 ; year:2012 ; pages:1-37 ; date:9.2012
Journal of high energy physics ; 2012, Heft 9 (25.9.2012), 1-37, 9.2012

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP09(2012)112

URN: urn:nbn:de:101:1-2019080121573435363256

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

Last update: 15.08.2025, 7:26 AM CEST

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

$Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV$

Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV

$Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$$

Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

$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$

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

$Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]$

Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

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

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$Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]$

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

$Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV$

Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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

$Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV$

Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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 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

$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

$Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV$

Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV

$Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$$

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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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$Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]$

Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

$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

$Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]$

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

$Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV$

Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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

$Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV$

Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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 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

$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

$Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV$

Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV

$Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$$

Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

$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$

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

$Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]$

Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

$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

$Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]$

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

$Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV$

Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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

$Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV$

Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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 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

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

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Other Objects (12)

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

Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV

Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

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

Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

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

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV

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

Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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 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

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

Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV

Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

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

Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

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

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV

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

Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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 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

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

Relative particle yield fluctuations in $$\text Pb--Pb }$$ Pb--Pb collisions at $$\sqrt{s_\mathrm{{NN}}} =2.76\hbox { TeV}$$ sNN=2.76TeV

Suppression and azimuthal anisotropy of prompt and nonprompt $\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

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

Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

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

Measurement of D s + production and nuclear modification factor in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

Addendum to: Centrality dependence of high-pT D-meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV

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

Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at s N N : = 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ 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 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

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