There is one more fundamental force in the Standard Model: the strong force. We have already met this force, as the force that keeps the nucleus together, but we discussed it before we knew that protons and neutrons are made of quarks. Now we need a force to keep quarks together inside the nucleons, and quark confinement tells us it must be a very strong force indeed. It is this force that, in modern parlance, is called the strong force and considered fundamental. The force between nucleons is a side effect of these more fundamental interactions among quarks.
Like all three forces in the Standard Model, the strong force is explained by a gauge theory, this time with gauge group , the color symmetry group of the quarks. The picture is simpler than that of electromagnetism and the weak force, however, because this symmetry is `unbroken'.
By now you can guess how this goes. Every kind of quark spans the
of . For example, the
left-handed up quark, with its three colors, lives in
The quarks interact by the exchange of gluons, the gauge bosons of the strong force. These gauge bosons live in , the complexified adjoint representation of . The interactions are drawn as Feynman diagrams, which now depict intertwining operators between representations of :
|Weak force||and bosons||, and|
On the other hand, the leptons are `white': they transform trivially under . So, they do not exchange gluons. In other words, they are not affected by the strong force. We can capture all of this information in a table, where we give the representations in which all our fermions live.
|The First Generation of Fermions -- Representations|
|Left-handed up quarks|
|Left-handed down quarks|
|Right-handed up quarks|
|Right-handed down quarks|