The earliest efforts to understand the interaction potential between nucleons followed Yukawa by working in terms of meson exchange. In other words the various mesons were considered the bosons of the strong interaction. The nucleon-nucleon interaction displays obvious physical analogies to the atom-atom interaction! |
The big problem with this
approach to the nucleon-nucleon interaction is that the
potential energy turns out to depend on absolutely
everything it could possibly depend upon! Things
quickly get insanely complex. |
The tensor term breaks rotational symmetry! |
Left: symmetric: TE, S = 1, T = 0 (d) and SE, S = 0, T = 1. Right: antisymmetric: SO, S = 0, T = 0, and TO, S = 1, T = 1. |
Glueballs, predicted "bound" states consisting only of gluons, have been predicted using approximations to the Standard Model, but have never been observed. If they existed they would be very massive and have an extremely short lifetime.
Note that it is essentially impossible to have a "free gluon." Gluons only exist as virtual particles, never real. Attempts to knock out quarks or gluons from a proton using very high energy electrons result in "jets" of hadrons... the quarks and gluons cease to exist as such, as they leave the proton interior.
Largely ignored by textbooks, there have been a
huge number of different so-called “bag models,” of the
nucleon and its excited states, proposed since the 1970s. All
the models confine three free valence quarks inside a
surface or spherical box of some kind, with various
different boundary conditions at, and couplings to, the
surface. People are still working on various complex bag
systems, but it is hard to see how any real basic physical
insight can result, although various basic symmetry principles
can be applied in creating a bag system. All bag models
stem from a very simple model originally suggested by
Bogoliubov in 1967. Research using bag models continues
even today (2022), with the latest wrinkles being chiral bag
models, and bag models for mesons.
The so-called Standard Model consists of Quantum Chromodynamics, the theory of the strong interaction, and the Electroweak Theory, the theory of electromagnetic and weak processes. No flaw in the model has yet shown up; experimental results support the Standard Model to high precision. However, one obvious problem is that it contains 26 parameters that must be put in "by hand," based on experimental results, with no justification from some deeper theory. Parameters of the Standard Model.