Binary Boosts
| dc.creator | Haeckl, R. | |
| dc.creator | Hund, V. | |
| dc.creator | Pilkuhn, H. | |
| dc.date | 1996-05-14 | |
| dc.date.accessioned | 2026-07-07T03:59:15Z | |
| dc.date.available | 2026-07-07T03:59:15Z | |
| dc.description | The relativistic motion of an isolated two--body system (bound or unbound) of given lab energy $K^{0}$ in QED is separated into cms motion and relative motion. The relative motion equation ${\cal K}_{L} ψ_{L} ({\bf r}_{L} ) =0$ contains the momentum eigenvalue ${\bf K}$ of the cms motion. It is greatly simplified by a binary boost to the atomic rest frame, where $K^{0}$ and ${\bf K}$ appear only in a Lorentz--invariant combination. This boost is not a product of single--particle boosts, which are useful only for perturbative interactions. CPT--invariance is demonstrated, and orthogonality relations are derived. | |
| dc.description | revtex, 10 pages, no figures The complete paper, including figures, is also available via anonymous ftp at ftp://www-ttp.physik.uni-karlsruhe.de/ or via www at http://www-ttp.physik.uni-karlsruhe.de/cgi-bin/preprints/ | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9605307 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9605307 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/46149 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | Atomic Physics | |
| dc.title | Binary Boosts | |
| dc.type | text |