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I understand (I may be wrong) that the highest density material is that of a quark-gluon plasma, such as the interior of a neutron star. Is there an upper limit to this density and is it known?
mathman said:I understand (I may be wrong) that the highest density material is that of a quark-gluon plasma, such as the interior of a neutron star. Is there an upper limit to this density and is it known?
kloptok said:According to our current understanding a black hole will form at some point if you keep increasing the density. The density where this happens would then be the upper limit for the density (and we are far from any such limit at today's colliders). Strongly interacting matter at these high densities is a question of current research. Some keywords to look for are "quark star", "quark matter", "color superconductivity", "color-flavor locking" and "QCD phase diagram".
mathman said:General relativity predicts that inside a black hole everything gets condensed to a point of infinite density. If there is an upper limit to the density of matter, then there would be a contradiction.
Well, there could be some modification of GR where quantum mechanics becomes relevant.stevebd1 said:Though I always thought that once inside the Schwarzschild radius, the world lines became space-like and there is no stable radius so no matter how much pressure the degenerate matter might exert, r is temporal and will not 'hold' and it's this that predicts the singularity (though in the case of the rotating black hole, time-like world lines are reinstated beyond the Cauchy horizon and matter may still exist in some form).
stevebd1 said:According to the paper in post 4, on page 62, a max density for quark stars appears to be 1500 MeV/fm3 and if my calculations are correct, this converts to about 2.674x1015 g/cm3. In this paper on page 4, the max appears to be approx 3.2x1015 g/cm3. According to another source-
'The maximum density of stable objects in hydrostatic equilibrium is 1016 g/cm3. This limit applies to any macroscopic object composed of standard model fermions'
which works out at 10 billion tonnes per cm3. Hypothetical Preon degenerate matter is suppose to occur at densities around 1020 g/cm3.
Though I always thought that once inside the Schwarzschild radius, the world lines became space-like and there is no stable radius so no matter how much pressure the degenerate matter might exert, r is temporal and will not 'hold' and it's this that predicts the singularity (though in the case of the rotating black hole, time-like world lines are reinstated beyond the Cauchy horizon and matter may still exist in some form).
mathman said:I understand (I may be wrong) that the highest density material is that of a quark-gluon plasma, such as the interior of a neutron star. Is there an upper limit to this density and is it known?
Hornbein said:The current belief is that neutron stars do not contain quark-gluon plasmas. A neutron star interior is much colder than the quark-gluon plasmas created at CERN.
I don't see why there should be an upper limit on density of small objects, though such density might be very transitory.
dauto said:There is no contradiction. The limit is for the density of stable matter in hydrostatic equilibrium. These conditions do not apply to interior of a black hole.
mathman said:My understanding is that there is no good theory describing the interior of a black hole.
dauto said:That's not right.Both GR and QM seem to work fine both inside and outside of the B-hole, except near the singularity at the center.
mathman said:That is a big exception!
Density in the context of quark-gluon plasma refers to the number of quarks and gluons per unit volume. It is a measure of how closely packed the particles are in the plasma state.
The density of quark-gluon plasma can be measured using various techniques such as heavy ion collisions, particle scattering experiments, and lattice QCD simulations. These methods involve analyzing the energy and momentum distribution of the particles to determine their density.
The density of quark-gluon plasma is influenced by several factors, including temperature, pressure, and the number of quarks and gluons present. It is also affected by the strength of the interactions between the particles, which can be altered by changing the energy or momentum of the system.
The density of quark-gluon plasma increases with temperature. This is because as the temperature rises, more energy is available to break the bonds between quarks and gluons, leading to a higher number of particles in the plasma state.
Studying the density of quark-gluon plasma is crucial for understanding the properties of matter at extremely high temperatures and densities, such as those present in the early universe. It also provides insights into the behavior of strongly interacting systems and can help us develop a better understanding of the fundamental forces of nature.