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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: Online-Ressource

Language: Englisch

Event: Veröffentlichung

(where): Aachen

(who): Universitätsbibliothek der RWTH Aachen

(when): 2018

Creator: Sirunyan, Albert M.

Contributor: CMS Collaboration

DOI: 10.18154/RWTH-2024-09389

URN: urn:nbn:de:101:1-2411060103193.310470476807

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:21 AM CEST

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Associated

Sirunyan, Albert M.
CMS Collaboration
Universitätsbibliothek der RWTH Aachen

Time of origin

2018

Other Objects (12)

$Measurement of B$^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

$Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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

$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

$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

$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$

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

$First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 TeV$

First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 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

$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

Hochschulschrift

Anisotropic flow of the charmed D*+ meson in non-central Pb-Pb collisions at sqrtsNN = 2.76 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

$Measurement of B$^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

$Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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

$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

$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

$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$

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

$First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 TeV$

First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 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

$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

Hochschulschrift

Anisotropic flow of the charmed D*+ meson in non-central Pb-Pb collisions at sqrtsNN = 2.76 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

$Measurement of B$^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

$Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV$

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ 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

$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

$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

$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$

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

$First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 TeV$

First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 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

$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

Hochschulschrift

Anisotropic flow of the charmed D*+ meson in non-central Pb-Pb collisions at sqrtsNN = 2.76 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

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

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Other Objects (12)

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

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

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

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

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

First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 TeV

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

Anisotropic flow of the charmed D*+ meson in non-central Pb-Pb collisions at sqrtsNN = 2.76 TeV

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

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

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

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

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

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

First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 TeV

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

Anisotropic flow of the charmed D*+ meson in non-central Pb-Pb collisions at sqrtsNN = 2.76 TeV

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

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

Centrality dependence of high-pT D meson suppression in Pb-Pb collisions at s N N : = 2.76 $$ \sqrts_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV

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

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

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

First measurements of N-subjettiness in central Pb-Pb collisions at s NN $$ \sqrts_{\mathrm{NN}}} $$ = 2.76 TeV

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

Anisotropic flow of the charmed D*+ meson in non-central Pb-Pb collisions at sqrtsNN = 2.76 TeV

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

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