Measurement of electrons from beauty-hadron decays in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV and Pb-Pb collisions at s N N = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

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Alternative title: 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV and Pb-Pb collisions at s N N
2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ TeV

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Measurement of electrons from beauty-hadron decays in p-Pb collisions at s N N ; volume:2017 ; number:7 ; day:11 ; month:7 ; year:2017 ; pages:1-40 ; date:7.2017
Journal of high energy physics ; 2017, Heft 7 (11.7.2017), 1-40, 7.2017

Classification: Physik

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP07(2017)052

URN: urn:nbn:de:1111-201708048837

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:20 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$

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

$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

$J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

$Measurement of B$^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

$Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Jet shapes of isolated photon-tagged jets in PbPb and pp collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV$

Jet shapes of isolated photon-tagged jets in PbPb and pp 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$

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

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$

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

$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

$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

$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

$J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

$Measurement of B$^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

$Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Jet shapes of isolated photon-tagged jets in PbPb and pp collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV$

Jet shapes of isolated photon-tagged jets in PbPb and pp 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$

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

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$

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

$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

$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

$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

$J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 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

$Measurement of B$^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

$Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV$

Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

$Jet shapes of isolated photon-tagged jets in PbPb and pp collisions at $\sqrts_\mathrm{NN}} =$ 5.02 TeV$

Jet shapes of isolated photon-tagged jets in PbPb and pp 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$

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

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$

Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at sNN=5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ and 2.76 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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Measurement of electrons from beauty-hadron decays in p-Pb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{NN}}}=5.02 $$ TeV and Pb-Pb collisions at s N N = 2.76 $$ \sqrts_{\mathrm{NN}}}=2.76 $$ 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

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

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Nuclear modification of $\Upsilon$ states in pPb 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

Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Jet shapes of isolated photon-tagged jets in PbPb and pp 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

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

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

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

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Nuclear modification of $\Upsilon$ states in pPb 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

Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Jet shapes of isolated photon-tagged jets in PbPb and pp 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

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

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

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

Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N : = 5.02 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV

J/ψ elliptic and triangular flow in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Nuclear modification of $\Upsilon$ states in pPb 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

Non-linear flow modes of identified particles in Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 5.02 TeV

Jet shapes of isolated photon-tagged jets in PbPb and pp 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

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

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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