A colloquial term for a state of matter where quarks are not confined within hadrons, as in a quark-gluon plasma.A colloquial term for a state of matter where quarks are not confined within hadrons, as in a quark-gluon plasma. This is an extreme state of matter that existed in the early universe just after the Big Bang, and can be recreated in particle accelerators by colliding heavy ions at relativistic speeds. In this state, quarks and gluons move freely over distances larger than the size of a proton.
The concept of quark-gluon plasma was proposed in the 1970s, and first experimental evidence was obtained at CERN in 2000, followed by more detailed studies at RHIC and the LHC.
Under normal conditions, quarks are permanently bound inside protons and neutrons by the strong nuclear force. At temperatures exceeding about 2 trillion kelvin, the energy density becomes so high that the confinement breaks down, and quarks and gluons form a plasma. This transition is analogous to how ice melts into liquid water, but for the fundamental constituents of matter.
Studying quark-gluon plasma helps physicists understand the strong force and the early evolution of the universe, and it is a key research area at particle accelerators.
The temperature of quark-gluon plasma created at the LHC reaches about 5.5 trillion kelvin, making it the hottest matter ever created in a laboratory.


