Abstract
It is shown that a relativistic basis for invariance under exists only if the group structure is extended to for any interaction terms. The notion of an inhomogeneous extension is introduced. This extension leaves the kinetic-energy terms invariant, though it still does not provide a fully satisfactory theory.
- Received 10 December 1964
DOI:https://doi.org/10.1103/PhysRev.138.B420
©1965 American Physical Society