Pseudorapidity distributions of charged hadrons in proton-lead collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 8.16 TeV

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Alternative title: 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 8.16 TeV

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Pseudorapidity distributions of charged hadrons in proton-lead collisions at s N N ; volume:2018 ; number:1 ; day:11 ; month:1 ; year:2018 ; pages:1-34 ; date:1.2018
Journal of high energy physics ; 2018, Heft 1 (11.1.2018), 1-34, 1.2018

Classification: Physik

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP01(2018)045

URN: urn:nbn:de:1111-2018032111115

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:59 AM CEST

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

$Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Pseudorapidity distributions of charged hadrons in proton-lead collisions at √sNN : = 5.02 and 8.16 TeV

$Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV$

Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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

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

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

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 inclusive J/ψ production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV$

Centrality dependence of inclusive J/ψ production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

$Λ c+ production in pp collisions at s=7 $$ \sqrts}=7 $$ TeV and in p-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV$

Λ c+ production in pp collisions at s=7 $$ \sqrts}=7 $$ TeV and in p-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

$Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV$

Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV

$Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrts_\mathrm{NN}}$ = 5.02 TeV$

Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrts_\mathrm{NN}}$ = 5.02 TeV

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Centrality and pseudorapidity dependence of the transverse energy density in pPb collisions at $\sqrts_\mathrm{NN}}=$ 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

$Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Pseudorapidity distributions of charged hadrons in proton-lead collisions at √sNN : = 5.02 and 8.16 TeV

$Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV$

Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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

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

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

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

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$Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV$

Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV

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$Centrality and pseudorapidity dependence of the transverse energy density in pPb collisions at $\sqrts_\mathrm{NN}}=$ 5.02 TeV$

Centrality and pseudorapidity dependence of the transverse energy density in pPb collisions at $\sqrts_\mathrm{NN}}=$ 5.02 TeV

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

$Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Pseudorapidity distributions of charged hadrons in proton-lead collisions at √sNN : = 5.02 and 8.16 TeV

$Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV$

Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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

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

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

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 inclusive J/ψ production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV$

Centrality dependence of inclusive J/ψ production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

$Λ c+ production in pp collisions at s=7 $$ \sqrts}=7 $$ TeV and in p-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV$

Λ c+ production in pp collisions at s=7 $$ \sqrts}=7 $$ TeV and in p-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

$Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV$

Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV

$Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrts_\mathrm{NN}}$ = 5.02 TeV$

Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrts_\mathrm{NN}}$ = 5.02 TeV

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Pseudorapidity distributions of charged hadrons in proton-lead collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 8.16 TeV

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Centrality and pseudorapidity dependence of the transverse energy density in pPb collisions at $\sqrts_\mathrm{NN}}=$ 5.02 TeV

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

Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Pseudorapidity distributions of charged hadrons in proton-lead collisions at √sNN : = 5.02 and 8.16 TeV

Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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

W and Z boson production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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 inclusive J/ψ production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Λ c+ production in pp collisions at s=7 $$ \sqrts}=7 $$ TeV and in p-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV

Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrts_\mathrm{NN}}$ = 5.02 TeV

Centrality and pseudorapidity dependence of the transverse energy density in pPb collisions at $\sqrts_\mathrm{NN}}=$ 5.02 TeV

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

Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Pseudorapidity distributions of charged hadrons in proton-lead collisions at √sNN : = 5.02 and 8.16 TeV

Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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

W and Z boson production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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 inclusive J/ψ production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Λ c+ production in pp collisions at s=7 $$ \sqrts}=7 $$ TeV and in p-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV

Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrts_\mathrm{NN}}$ = 5.02 TeV

Centrality and pseudorapidity dependence of the transverse energy density in pPb collisions at $\sqrts_\mathrm{NN}}=$ 5.02 TeV

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

Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Pseudorapidity distributions of charged hadrons in proton-lead collisions at √sNN : = 5.02 and 8.16 TeV

Prompt Λ c + production in pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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

W and Z boson production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ 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 inclusive J/ψ production in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Λ c+ production in pp collisions at s=7 $$ \sqrts}=7 $$ TeV and in p-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV

Energy dependence of exclusive $$\mathrm J}/\psi $$ J/ψ photoproduction off protons in ultra-peripheral p–Pb collisions at $$\sqrts_{\mathrm \scriptscriptstyle NN}}} : = 5.02$$ sNN=5.02 TeV

Nuclear modification of $\Upsilon$ states in pPb collisions at $\sqrts_\mathrm{NN}}$ = 5.02 TeV

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