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Measurement of $\Xi_c^0$ production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV

$\Xi_c^0$ baryon production cross section in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
Energy
5.02 TeV
System
p-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
xic0_ppb_vs_pp_5_tev.eps
Figure image (.pdf)
xic0_ppb_vs_pp_5_tev.pdf
Invariant-mass distribution of $\Xi_c^0$ in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
Energy
5.02 TeV
System
p-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
invmassfitxic0.eps
Figure image (.pdf)
invmassfitxic0.pdf
Acceptance x efficiency as a function of 𝑝T for $\Xi_c^0$ baryons
Energy
5.02 TeV
System
p-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
efficiency_0.eps
Figure image (.pdf)
efficiency_0.pdf
Nuclear modification factor of the $\Xi_c^0$ baryon in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
Energy
5.02 TeV
System
p-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
rppb.eps
Figure image (.pdf)
rppb.pdf
$\Xi_c^0$/$D^0$ production cross section ratio as a function of 𝑝T in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
Energy
5.02 TeV
System
p-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
xic0_d0_ratio.eps
Figure image (.pdf)
xic0_d0_ratio.pdf
$\Xi_c^0$/$\Lambda_c^+$ production cross section ratio as a function of 𝑝T in p–Pb collisions at $\sqrt{s_\mathrm{NN}}= 5.02$ TeV
Energy
5.02 TeV
System
p-Pb
Scope: PWG
PWG-HF (Heavy Flavour)
Figure image (.eps)
xic0vslam.eps
Figure image (.pdf)
xic0vslam.pdf