Rotations and e, $ν$ Propagators, Part II
| dc.creator | Shurtleff, Richard | |
| dc.date | 2000-07-31 | |
| dc.date.accessioned | 2026-07-07T04:10:15Z | |
| dc.date.available | 2026-07-07T04:10:15Z | |
| dc.description | We continue to derive spacetime quantities and spin 1/2 propagators from rotations. Rotation-invariant projection operators are found for each element of a four element basis, i.e. a basis for four component quantities with specific transformation rules under rotations. With these four projection operators, we make two spacetime invariant projection operators, i.e. once space, time, energy, and momentum are identified. The spacetime invariant operators are propagators for free neutrinos. Except for the substitute basis, the process is the same as the one that gave electron propagators in Part I. PACS number(s): 11.30.-j, 11.30.Cp, and 03.65.Fd | |
| dc.description | 8 pages, no figures, LaTex | |
| dc.identifier | https://arxiv.org/abs/hep-th/0007245 | |
| dc.identifier | http://arxiv.org/abs/hep-th/0007245 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/50156 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Rotations and e, $ν$ Propagators, Part II | |
| dc.type | text |