  The spectroscopic properties of heavy quarkonia are substantially different
in the quark-gluon plasma (QGP) that is created in relativistic heavy-ion
collisions as compared to the vacuum situation that can be tested in pp
collisions at the same center-of-mass energy. In this article, a series of
recent works about the dissociation of the Y(nS) and chi_b(nP) states in the
hot QGP is summarized. Quarkonia dissociation occurs due to (1) screening of
the real quark-antiquark potential, (2) collisional damping through the
imaginary part of the potential, and (3) gluon-induced dissociation. In
addition, reduced feed-down plays a decisive role for the spin-triplet ground
state. Transverse-momentum and centrality-dependent data are well reproduced in
Pb-Pb collisions at LHC energies. In the asymmetric p-Pb system, alterations of
the parton density functions in the lead nucleus account for the leading
fraction of the modifications in cold nuclear matter (CNM), but the hot-medium
effects turn out to be relevant in spite of the small initial spatial extent of
the fireball, providing additional evidence for the generation of a quark-gluon
droplet.
