
An instanton is a non-perturbative solution in quantum field theory that describes tunneling effects between vacua or entanglement phenomena.Instantons are non-perturbative solutions of field equations in Euclidean spacetime. They describe tunneling transitions between vacuum states of gauge theories, such as quantum chromodynamics. An instanton is localized: its action is concentrated in a limited region and over a short time interval, hence the name (from instant). Summing over instantons provides a contribution to physical quantities that is inaccessible through ordinary perturbation theory.
The concept of the instanton emerged in 1975 in the works of Alexander Polyakov and collaborators, but its roots go back to the study of tunneling in double-well quantum mechanics. In 1976, Gerard 't Hooft computed the instanton-induced interaction of quarks. The solution of the Yang-Mills equations in Euclidean space had been found earlier—the Belavin-Polyakov-Tyupkin instanton (BPST, 1975). In the 1980s, instanton methods were applied to electroweak theory, where they predict baryon number violation.
The instanton action S = 8π²/g², where g is the gauge coupling constant. The tunneling amplitude is proportional to e^{-S}, so at small g the instanton contribution is exponentially suppressed, but becomes significant at large g (in the infrared regime of QCD). In the path integral, transitioning to Euclidean time (τ = it) turns oscillating exponentials into decaying ones, making the tunneling path the 'most probable'. The instanton solution is self-dual: F = ±*F, which guarantees saturation of the Bogomolny bound and minimum action. For calculations, the 't Hooft ansatz is used, summing configurations with many instantons and anti-instantons (instanton gas). The tunneling effect is described similarly, but with imaginary time.
Calculations with instantons explain why neutrons and protons hold together so tightly, and help understand how the void is structured at the micro level.
It is instantons that are responsible for the η' meson being noticeably heavier than other light mesons.





















