The quantum field theory describing the strong interaction between quarks and gluons.Quantum chromodynamics (QCD) is the quantum field theory that describes the strong nuclear force, which binds quarks and gluons into protons, neutrons, and other hadrons. It is one of the two pillars of the Standard Model of particle physics, alongside the electroweak theory. QCD explains why quarks are never found in isolation but are confined inside composite particles, and it governs the behavior of nuclear matter under extreme conditions, such as in neutron stars or the early universe.
QCD was developed in the early 1970s by Harald Fritzsch, Heinrich Leutwyler, and Murray Gell-Mann, building on the quark model and the discovery of asymptotic freedom by David Gross, Frank Wilczek, and H. David Politzer in 1973.
QCD is a gauge theory based on the symmetry group SU(3), with six flavors of quarks carrying a 'color' charge (red, green, or blue) and eight massless gluons mediating the force. The theory's most striking feature is asymptotic freedom: at very short distances (high energies), the force between quarks weakens, allowing them to behave almost freely. At larger distances, the force strengthens, confining quarks into colorless bound states. This behavior is described by the running coupling constant and is calculated using lattice QCD or perturbative methods.
QCD is essential for understanding particle collisions at accelerators like the LHC, predicting the properties of quark-gluon plasma, and modeling the interior of neutron stars.
The strong force is so strong that the energy needed to separate two quarks is enough to create a new quark-antiquark pair, which is why free quarks are never observed.










