J/ψ production as a function of charged-particle multiplicity in p-Pb collisions at $$ \sqrt{s_{\mathrm{NN}}} $$ = 8.16 TeV

  title={J/$\psi$ production as a function of charged-particle multiplicity in p-Pb collisions at \$\$ \sqrt\{s\_\{\mathrm\{NN\}\}\} \$\$ = 8.16 TeV},
  author={Alice Collaboration},
Inclusive J/$\psi$ yields and average transverse momenta in p-Pb collisions at a center-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}$ = 8.16 TeV are measured as a function of the charged-particle pseudorapidity density with ALICE. The J/$\psi$ mesons are reconstructed at forward $(2.03<y_{\rm cms}<3.53)$ and backward ($-4.46<y_{\rm cms}<-2.96$) center-of-mass rapidity in their dimuon decay channel while the charged-particle pseudorapidity density is measured around midrapidity. The J… Expand

Figures and Tables from this paper


Double, triple, and $n$-parton scatterings in high-energy proton and nuclear collisions
The framework to compute the cross sections for the production of particles with high mass and/or large transverse momentum in double- (DPS), triple- (TPS), and in general $n$-parton scatterings,Expand
The quest for the quark–gluon plasma
Experiments at the Large Hadron Collider should consolidate the evidence for this exotic medium's existence, and allow its properties to be characterized. Expand
The EvtGen particle decay simulation package
With several new B-physics experiments now taking data, the physics of B-meson decays will be studied in greater detail than previously possible. It is important to have a simulation of theExpand
The Monte Carlo Event Generator DPMJET-III
A new version of the Monte Carlo event generator DPMJET is presented. It is a code system based on the Dual Parton Model and unifies all features of the DTUNUC-2, DPMJET-II and PHOJET1.12 eventExpand
PHOTOS - a universal Monte Carlo for QED radiative corrections: version 2.0
This paper documents an update of the PHOTOS algorithm, by E. Barberio, B. van Eijk and Z. Was, for the Monte Carlo simulation of QED photon radiative corrections in decays. The algorithm isExpand
$J/\psi$ Suppression by Quark-Gluon Plasma Formation
If high energy heavy ion collisions lead to the formation of a hot quark-gluon plasma, then colour screening prevents ce binding in the deconfined interior of the interaction region. To study thisExpand