Abstract
We show that in all theories with a Lorentz-covariant energy-momentum tensor, such as all known renormalizable quantum field theories, composite as well as elementary massless particles with j 〉 1 are forbidden. Also, in all theories with a Lorentz-covariant conserved current, such as renormalizable theories with a symmetry that commutes with all local symmetries, there cannot exist composite or elementary particles with nonvanishing values of the corresponding charge and j 〉 1/2.
| Original language | English (US) |
|---|---|
| Pages (from-to) | 59-62 |
| Number of pages | 4 |
| Journal | "Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics" |
| Volume | 96 |
| Issue number | 1-2 |
| DOIs | |
| State | Published - 1980 |
| Externally published | Yes |
All Science Journal Classification (ASJC) codes
- Nuclear and High Energy Physics