Abstract
It is shown that the interaction of a massive fermion with massless gauge bosons is automatically parity-conserving even when the whole theory does not conserve parity. This explains the parity-invariance of the strong and electromagnetric interactions.
| Original language | English |
|---|---|
| Pages (from-to) | 204-206 |
| Number of pages | 3 |
| Journal | Physica Scripta |
| Volume | 34 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - 1986 Sept 1 |