Bottomonium suppression at RHIC and LHC
arXiv:1807.07452 · doi:10.1016/j.nuclphysa.2018.09.034
Abstract
The strong suppression of heavy quarkonia is a good indicator that one has generated a quark-gluon plasma (QGP) in an ultrarelativistic heavy ion collision. Recent advancements in first principles calculations of the heavy quark potential provide additional insight into this suppression and can be used to further pin down the in-medium properties of the QGP. Realistic 3+1d dissipative hydrodynamical models can be used to simulate the QGP and, with bottomonium as a probe, one can make inferences for the initial temperature of the QGP and other phenomenological parameters such as the shear viscosity to entropy density ratio. However, progressing to LHC TeV Pb-Pb collisions, one expects regeneration to have an increasingly important impact on the suppression observables. In this proceedings, we present a brief overview to set up the model and then provide model results for bottomonium suppression and regeneration, for ultrarelativistic heavy-ion collision experiments at RHIC and LHC.
4 pages, 6 figures; proceedings contribution to Quark Matter 2018, May 13-19 2018
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Cited by in corpus (7)
- Quantum evolution of quarkonia with correlated and uncorrelated noise
- Heavy quarkonia spectroscopy at zero and finite temperature in bottom-up AdS/QCD
- Anisotropic escape mechanism and elliptic flow of bottomonia
- Fireball tomography from bottomonia elliptic flow in relativistic heavy-ion collisions
- Bottomonium suppression in PbPb collision at energies available at the CERN large hadron collider
- Quarkonium: a theory overview
- Production of bottomonia states in proton+proton and heavy-ion collisions