When the transformation between bases in a phenomenological theory is anomalous, the theories are not equivalent, but can be made so by the addition of an appropriate anomaly functional. This functional can be given a simple form which allows the derivation of a sufficient condition for the impossibility of anomaly cancellation.
|Original language||English (US)|
|Number of pages||10|
|Journal||Nuclear Physics, Section B|
|State||Published - Aug 27 1984|
All Science Journal Classification (ASJC) codes
- Nuclear and High Energy Physics