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]]

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Alternative title: 2.76 $$ \sqrt{\mathrm{s}}_{\mathrm{NN}}}=2.76 $$ TeV [[electronic resource]]

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Transverse momentum dependence of D-meson production in Pb-Pb collisions at s N N ; volume:2016 ; number:3 ; day:14 ; month:3 ; year:2016 ; pages:1-43 ; date:3.2016
Journal of high energy physics ; 2016, Heft 3 (14.3.2016), 1-43, 3.2016

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2016)081

URN: urn:nbn:de:1111-2016032410495

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 11:01 AM CEST

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$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

$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}

$Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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]]

$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

$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 $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

$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

$Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV$

Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV

$Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

$Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV$

Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV

$Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV$

Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

$Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC$

Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC

$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

$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}

$Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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]]

$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

$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 $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

$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

$Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV$

Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV

$Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

$Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV$

Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV

$Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV$

Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

$Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC$

Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC

$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

$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}

$Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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]]

$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

$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 $\sqrt{s_{_{\text NN}}}}} =2.76$ $\,\mathrmTeV}$

$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

$Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV$

Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV

$Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

$Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV$

Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV

$Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV$

Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

$Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC$

Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC

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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]]

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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

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

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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]]

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

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

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

Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV

Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV

Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC

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

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

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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]]

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

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

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

Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV

Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV

Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC

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

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

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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]]

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

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

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

Neutral pion production at midrapidity in pp and Pb–Pb collisions at $$\sqrts_{{\mathrm NN}}}}= 2.76\,\mathrm TeV}}$$ s NN : = 2.76 TeV

Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

Measurement of $$\Upsilon } $$ Υ production in $${\mathrm p}}} {\mathrm p}}} $$ p p collisions at $$\sqrt{s}} =2.76\mathrm \,TeV}} $$ s : = 2.76 TeV

Elliptic flow of identified hadrons in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

Measurement of jet fragmentation in Pb+Pb and pp collisions at $$\sqrt{s_\mathrm{NN}}} : = 2.76$$ s NN = 2.76 TeV with the ATLAS detector at the LHC

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