Abstract
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) |
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Pages (from-to) | 55-64 |
Number of pages | 10 |
Journal | Nuclear Physics, Section B |
Volume | 243 |
Issue number | 1 |
DOIs | |
State | Published - Aug 27 1984 |
Externally published | Yes |
All Science Journal Classification (ASJC) codes
- Nuclear and High Energy Physics