In
the study of the basic interactions which exist in nature, one of the
most intriguing is the strong nuclear interaction. An important
property of the strong interaction is that quarks and gluons are
never seen in isolation, a phenomenon called "confinement".
Such behavioural changes happen when the nuclear matter is heated to
the extreme conditions. The "deconfined" quarks and gluons
hence form a new state of nuclear matter, which has been called the
Quark-Gluon Plasma (QGP). Just a few microseconds after the Big Bang, the universe is believed to have crossed the phase boundary,
condensing from a QGP to a hadron gas as the temperature decreased.
In the experimental front, producing the QGP in the laboratory and
studying its properties is the main goal of experiments with heavy-ion collisions at high-energies. Among the probes of the QGP,
the heavy quarks have generated interest due to their unique role in
the diagnostics of the highly excited medium created in the
relativistic heavy-ion collisions. Experimentally and theoretically,
over the two decades, the properties of heavy quarkonium states
(which are bound states of heavy quark-antiquark pairs, charmonium
and bottomonium) in a hot and dense QCD medium have been extensively
studied.
Link to the Summary
Link to the Summary
No comments:
Post a Comment