The strong interaction is the fundamental force that binds quarks together via gluons to form protons, neutrons, and other hadrons.The strong interaction is one of the four fundamental forces of nature. It is described by quantum chromodynamics (QCD), a theory based on color charges of quarks (analogous to electric charge but of three types: red, green, blue). Massless gluons carry the interaction between quarks and themselves carry color charge, making QCD highly nonlinear. Two key properties are confinement—quarks and gluons cannot exist freely; they are always locked inside hadrons (protons, neutrons, etc.)—and asymptotic freedom—at very short distances, the interaction weakens, and quarks behave almost as free particles.
The first indications of the strong interaction appeared in the 1920s with the discovery of the atomic nucleus. In 1935, Hideki Yukawa proposed the meson theory of nuclear forces. The development of accelerators in the 1950s–60s led to the discovery of many hadrons, necessitating the introduction of the quark model (Gell-Mann, Zweig) in 1964. The color degree of freedom and the confinement hypothesis were formulated in the early 1970s, and quantum chromodynamics as a gauge theory with SU(3) group was constructed by Gross, Wilczek, and Politzer in 1973 (Nobel Prize 2004). Experimental confirmation of asymptotic freedom came from deep inelastic scattering.
The strong interaction binds quarks through the exchange of gluons. Gluons are massless but carry color, so they interact with each other, forming 'gluon chains' and strings. When trying to separate quarks, the potential energy of the string increases, and upon exceeding the threshold for pair production of quark-antiquark, the string breaks with the formation of new hadrons—this phenomenon is hadronization. In high-energy collisions, quarks and gluons form quark-gluon plasma—a state in which they are weakly bound. The residual strong interaction between colorless hadrons manifests as nuclear forces holding nucleons together in the nucleus (an effective interaction analogous to van der Waals forces in molecular physics). Accompanying laws: Pauli principle, gauge invariance, asymptotic freedom.
The energy of the strong interaction powers the Sun and stars through nuclear fusion, and is also used in nuclear reactors and potentially in future thermonuclear power plants.
The proton's mass is almost entirely (99%) due not to the masses of its constituent quarks but to the energy of the gluon field that holds them together—that is, according to the famous formula E=mc², the binding energy manifests itself as mass.
















