A gluon is a massless gauge boson that mediates the strong force between quarks in quantum chromodynamics.Gluons are invisible threads that glue quarks in protons and neutrons, like superglue. Without them all matter would crumble into dust.
The concept of gluons emerged with quantum chromodynamics in the early 1970s. The works of Gross, Wilczek, and Politzer (Nobel Prize 2004) demonstrated the property of asymptotic freedom, explaining the weakness of interaction at short distances. First experimental confirmation was obtained in 1979 at DESY (Hamburg) by observing three-jet events in e⁺e⁻ annihilation. Later, gluon properties were studied in detail at LEP, HERA, and LHC colliders.
The gluon field is described by the tensor G_{μν}^a within QCD with the gauge group SU(3). The Lagrangian contains gluon self-interaction terms (triple and quartic vertices), which leads to saturation of the gluon field at high energies and confinement. The exchange of gluons between quarks generates a force whose potential grows linearly with distance: V(r) ~ kr. When trying to isolate a color charge, the field energy reaches the threshold for quark-antiquark pair production, leading to hadronization and jet formation. Asymptotic freedom ensures that at ultra-short distances the interaction weakens, allowing the application of perturbation theory.
Gluons are so sticky that they cling not only to quarks but also to each other! This makes the strong interaction very unusual.















