Multiplicity and event-scale dependent flow and jet fragmentation in pp collisions at s $$ \sqrts} $$ = 13 TeV and in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

Umfang: 1 Online-Ressource.

Sprache: Englisch

Erschienen in: Multiplicity and event-scale dependent flow and jet fragmentation in pp collisions at s $$ \sqrts} $$ = 13 TeV and in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV ; volume:2024 ; number:3 ; day:15 ; month:3 ; year:2024 ; pages:1-35 ; date:3.2024
Journal of high energy physics ; 2024, Heft 3 (15.3.2024), 1-35, 3.2024

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2024)092

URN: urn:nbn:de:101:1-2405211122501.294784614104

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

Letzte Aktualisierung: 14.08.2025, 10:49 MESZ

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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$

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

$Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

$Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV$

Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV

$Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV$

Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV

$Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV$

Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV

$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

$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

$Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV$

Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV

$(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 TeV$

(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 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

$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$

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

$Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

$Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV$

Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV

$Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV$

Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV

$Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV$

Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV

$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

$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

$Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV$

Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV

$(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 TeV$

(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 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

$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$

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

$Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

$Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV$

Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV

$Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV$

Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV

$Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV$

Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV

$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

$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

$Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV$

Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV

$(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 TeV$

(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 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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Multiplicity and event-scale dependent flow and jet fragmentation in pp collisions at s $$ \sqrts} $$ = 13 TeV and in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

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Ähnliche Objekte (12)

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

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV

Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV

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

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

Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV

(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 TeV

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

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

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV

Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV

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

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

Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV

(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 TeV

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

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

Z-boson production in p-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 8.16 TeV and Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

Thermal model description of p–Pb collisions at $$\sqrts_{NN}} = 5.02$$ sNN=5.02 TeV

Charged-particle multiplicity fluctuations in Pb–Pb collisions at $$\sqrts_{\mathrm NN}}}$$ s NN = 2.76 TeV

Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s $$ \sqrts} $$ , s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Measurement of $$\Lambda $$ Λ (1520) production in pp collisions at $$\sqrts} : = 7\ \hbox TeV}$$ s=7TeV and p–Pb collisions at $$\sqrts_{\mathrm{NN}}} = 5.02\ \hbox TeV}$$ sNN=5.02TeV

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

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

Anisotropic flow of identified hadrons in Xe-Xe collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.44 TeV

(Anti-)deuteron production in pp collisions at $$\sqrts}=13 \ \text TeV}$$ s = 13 TeV

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

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