quark-gluon

From the AdS/CFT correspondence (Maldacena), it's possible to calculate the ratio of viscosity to entropy in the quark-gluon plasma.

The Universe coalesced into hydrogen and helium from a quark-gluon plasma soon after the Big Bang.

So, changing the energy of a quark-gluon plasma doesn't have a huge effect on its entropy.

According to wikipedia (heh), quark-gluon plasma is not really a plasma so much as a liquid.

So in this case, quark-gluon-electron interactions are real, and basically everything else is like 99% imaginary.

The ratios can be traced back through the expansion to the quark-gluon soup stage.

I personally identify as a quark-gluon plasma held together by the strong force and a sheer lack a boundaries.

Specifically, they're looking at quark-gluon plasma from the heavy-ion collision at LHC.

And if you want to be exhaustive, don't forget the other oddball types: the high-density states like neutronium, the high-energy states like quark-gluon plasma, etc.

Similarly, it is for a quark-gluon plasma; thus, phenomenological models are used, like how the nuclear potential could look and the masses for different combinations of nuclei.

I don't want to get too far away from the main point but because of this, quarks are found (normally, outside of Big-Bang quark-gluon plasmas) in combination...

So it turns out the Philosopher's Stone is real, it just involves a 10,000-ton detection apparatus, a 17-mile-diameter accelerator tube as a source of prima, and a quark-gluon plasma.

Other recurring examples are "black holes" in the lab [1] and "AdS/CFT" (of string theory fame) in solid state and quark-gluon plasma physics [2].

If we include the quark-gluon plasma phase, we can just amend that to being supported by quark degeneracy pressure (and noting that "neutron" is just a special case of "quark" for this purpose).

Quark-gluon plasma occurs only at extreme energies, and in these collisions it is a essentially a chaos of quarks and gluons.