QED derived from the two-body interaction (2) The derivation
| dc.creator | Bell, Sarah B. M. | |
| dc.creator | Cullerne, John P. | |
| dc.creator | Diaz, Bernard M. | |
| dc.date | 2001-04-03 | |
| dc.date | 2002-11-27 | |
| dc.date.accessioned | 2026-07-07T06:01:52Z | |
| dc.date.available | 2026-07-07T06:01:52Z | |
| dc.description | We have shown in a previous paper that the Dirac bispinor can vary like a four-vector and that Quantum Electrodynamics (QED) can be reproduced with this form of behaviour.(2) We have also shown in part I (3) of this paper, that QED with the same transformational behaviour also holds in a second space which we called M-space. Here we use M-space to show that QED can be reduced to two simple rules for a two-body interaction. | |
| dc.description | 31 pages, references updated - no other changes | |
| dc.identifier | https://arxiv.org/abs/quant-ph/0104018 | |
| dc.identifier | http://arxiv.org/abs/quant-ph/0104018 | |
| dc.identifier | FOUND.PHYS.34(2),FEB.2004 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/89414 | |
| dc.subject | Quantum Physics | |
| dc.title | QED derived from the two-body interaction (2) The derivation | |
| dc.type | text |