Goldstone modes

From SklogWiki
Jump to navigation Jump to search
This article is a 'stub' page, it has no, or next to no, content. It is here at the moment to help form part of the structure of SklogWiki. If you add sufficient material to this article then please remove the {{Stub-general}} template from this page.

Goldstone modes (also known as Nambu-Goldstone bosons)[1] [2] arise from Goldstone's conjecture; that if there is continuous symmetry transformation under which the Lagrangian is invariant, then either the vacuum state is also invariant under the transformation, or there must exist spinless particles of zero mass.

See also[edit]

References[edit]

Related reading