Goldstone's theorem states that spontaneous symmetry breaking in a system leads to massless excitations called Goldstone bosons.In 1961, Jeffrey Goldstone developed the idea that spontaneous breaking of a continuous symmetry in quantum field theory leads to the appearance of massless scalar particles. In the 'Mexican hat' model (a potential with a degenerate minimum), the field rolls down to a specific point on the bottom, fixing the vacuum state. Excitations along the flat direction of the bottom correspond to Goldstone bosons — their mass is strictly zero thanks to the residual symmetry.
The idea appeared in the work of Yoichiro Nambu (1960) in the context of superconductivity, and the general formulation was given by Jeffrey Goldstone (1961) with contributions from Salam and Weinberg. Further development is associated with Peter Higgs and others, who showed how to avoid masslessness via the Higgs mechanism.
Goldstone bosons arise in systems from condensed matter to cosmology. Their mass is protected by symmetry: if the breaking is exact, the mass is zero; with explicit small breaking they become pseudo-Goldstone bosons with small mass. It is applied in the physics of pions, axions, and the Higgs mechanism.
These particles explain why sound waves appear in crystals, and spin waves (magnons) in magnets. They are also key to understanding the mass of elementary particles.
In the early universe, there apparently existed a symmetry between the weak and electromagnetic interactions. Its spontaneous breaking gave rise to Goldstone bosons that were 'eaten' by gauge fields, giving mass to the W and Z bosons — this trick was called the Higgs mechanism.












