Color charge is a quantum property of quarks and gluons that gives rise to the strong nuclear force.Color charge is a special property of quarks and gluons, like paint on balls. Only instead of paints there are three colors: red, green, and blue. It helps particles 'communicate' via the strong interaction.
The concept was introduced by Oscar Greenberg in 1964 to explain the symmetry of baryon wave functions. Soon Yoichiro Nambu and Han Moo-Young proposed using a triplet structure. The final formulation in the framework of QCD was completed in the 1970s, when asymptotic freedom was discovered and the role of SU(3) as an exact gauge symmetry was understood. Experimentally, the existence of color charge is confirmed by analysis of hadron production cross sections in e⁺e⁻ collisions (ratio R = σ(e⁺e⁻ → hadrons)/σ(e⁺e⁻ → μ⁺μ⁻)).
In QCD, each quark current changes color by emitting or absorbing a gluon. The interaction Lagrangian has the form g_s \bar{ψ} γ^μ t^a ψ A_μ^a, where t^a are the generators of SU(3) in the fundamental representation. Gluons themselves carry color, so their self-interaction leads to charge anti-screening: the effective coupling constant α_s increases with decreasing energy scale. This leads to confinement at distances of about 1 fm: the potential V(r) ≈ -4α_s/(3r) + σ r, where σ is the string tension. At high energies (small distances) α_s decreases (asymptotic freedom). Observed hadrons are always white (singlet under SU(3)).
Quarks constantly change their color, like chameleons in the jungle. But in nature we see only 'colorless' combinations — like light from three colored flashlight beams.
| c_app | variable | Apparent color index of a celestial object — color index |
| c_int | variable | Intrinsic color index of the object — color index |
| E | variable | Color excess due to interstellar extinction — color excess |












