Event-Shape Engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

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Alternative title: 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Event-Shape Engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at s N N ; volume:2019 ; number:2 ; day:22 ; month:2 ; year:2019 ; pages:1-36 ; date:2.2019
Journal of high energy physics ; 2019, Heft 2 (22.2.2019), 1-36, 2.2019

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2019)150

URN: urn:nbn:de:101:1-2019121723090891796562

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

Last update: 14.08.2025, 11:01 AM CEST

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D-meson azimuthal anisotropy in mid-central Pb–Pb collisions at √sNN = 5.02 TeV

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$Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 2.76 TeV$

Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 2.76 TeV

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Event-Shape Engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

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Other Objects (12)

Jet properties in PbPb and pp collisions at sNN=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 B$^0_\mathrms}$ meson production in pp and PbPb collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV

Measurement of B$^0_\mathrms}$ meson production in pp and PbPb collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV

D-meson azimuthal anisotropy in midcentral Pb–Pb collisions at √sNN = 5.02 TeV

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

D-meson azimuthal anisotropy in mid-central Pb–Pb collisions at √sNN = 5.02 TeV

D-meson azimuthal anisotropy in mid-central Pb–Pb collisions at √sNN = 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

Measurement of prompt D0 meson azimuthal anisotropy in PbPb collisions at √sNN : = 5.02 TeV

Measurement of the groomed jet mass in PbPb and pp collisions at s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 2.76 TeV

Jet properties in PbPb and pp collisions at sNN=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 B$^0_\mathrms}$ meson production in pp and PbPb collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV

Measurement of B$^0_\mathrms}$ meson production in pp and PbPb collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV

D-meson azimuthal anisotropy in midcentral Pb–Pb collisions at √sNN = 5.02 TeV

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

D-meson azimuthal anisotropy in mid-central Pb–Pb collisions at √sNN = 5.02 TeV

D-meson azimuthal anisotropy in mid-central Pb–Pb collisions at √sNN = 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

Measurement of prompt D0 meson azimuthal anisotropy in PbPb collisions at √sNN : = 5.02 TeV

Measurement of the groomed jet mass in PbPb and pp collisions at s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 2.76 TeV

Jet properties in PbPb and pp collisions at sNN=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 B$^0_\mathrms}$ meson production in pp and PbPb collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV

Measurement of B$^0_\mathrms}$ meson production in pp and PbPb collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV

D-meson azimuthal anisotropy in midcentral Pb–Pb collisions at √sNN = 5.02 TeV

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

D-meson azimuthal anisotropy in mid-central Pb–Pb collisions at √sNN = 5.02 TeV

D-meson azimuthal anisotropy in mid-central Pb–Pb collisions at √sNN = 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

Measurement of prompt D0 meson azimuthal anisotropy in PbPb collisions at √sNN : = 5.02 TeV

Measurement of the groomed jet mass in PbPb and pp collisions at s N N = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 2.76 TeV

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