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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: Online-Ressource, 1 online resource.

Language: Englisch

Bibliographic citation: 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 ; volume:2023 ; number:5 ; day:5 ; month:5 ; year:2023 ; pages:1-44 ; date:5.2023
Journal of high energy physics ; 2023, Heft 5 (5.5.2023), 1-44, 5.2023

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2023)036

URN: urn:nbn:de:101:1-2023110609304854627879

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

Last update: 14.08.2025, 10:58 AM CEST

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Other Objects (12)

$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

$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 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

$Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Underlying-event properties in pp and p–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

$Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV$

Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV

$Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Higher-order moments of the elliptic flow distribution 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$

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

$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 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

$Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Underlying-event properties in pp and p–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

$Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV$

Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV

$Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Higher-order moments of the elliptic flow distribution 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$

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

$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 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

$Underlying-event properties in pp and p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

Underlying-event properties in pp and p–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

$Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV$

Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV

$Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

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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

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Other Objects (12)

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

Anisotropic flow and flow fluctuations of identified hadrons in 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

Underlying-event properties in pp and p–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

Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Higher-order moments of the elliptic flow distribution 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

Anisotropic flow and flow fluctuations of identified hadrons in 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

Underlying-event properties in pp and p–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

Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Higher-order moments of the elliptic flow distribution 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

Anisotropic flow and flow fluctuations of identified hadrons in 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

Underlying-event properties in pp and p–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

Prompt and nonprompt ψ(2S) production in pPb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Higher-order moments of the elliptic flow distribution in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

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