algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)
quantum mechanical system, quantum probability
interacting field quantization
physics, mathematical physics, philosophy of physics
theory (physics), model (physics)
experiment, measurement, computable physics
Axiomatizations
Tools
Structural phenomena
Types of quantum field thories
In the standard model of particle physics, the hadrons, such as the proton, are supposedly bound states of three quarks, the latter being the fundamental objects in quantum chromodynamics. In fact, quarks are thought to be confined to such colour-charge-neutral bound states. However, at the relevant energy-scale QCD is “strongly coupled” (the coupling constant is large) so that established methods of perturbative quantum field theory do not apply (possibly standard pQFT has to be supplied with an interacting vacuum state, or more general methods of non-perturbative quantum field theory are needed, all of which remains open). As a result, the expected confinement of quarks to hadrons is theoretically an open problem, known in mathematical physics essentially as the mass gap problem.
Therefore, together with the very existence of hadrons, also their basic properties, such as mass and spin do not currently have a derivation from first principles in QCD. There exists qualitative understanding and there exists computer simulation in lattice QCD. When experiment showed that also these heuristics drastically failed to provide an understanding of the spin of the proton in terms of the spin of its constitutents quarks and of the gluons binding these quarks together, the situation was called the proton spin crisis or proton spin puzzle.
Anthony Thomas, The spin of the proton, Progress in Particle and Nuclear Physics Volume 61, Issue 1, July 2008, Pages 219–228 Quarks in Hadrons and Nuclei — 29th Course International Workshop on Nuclear Physics (arXiv:0805.4437)
Anthony Thomas, The resolution of the proton spin crisis, 2008 (pdf)
See also
Created on November 11, 2018 at 10:13:42. See the history of this page for a list of all contributions to it.