More about the S=1 relativistic oscillator
| dc.creator | Dvoeglazov, Valeri V. | |
| dc.date | 1998-01-11 | |
| dc.date.accessioned | 2026-07-07T04:24:05Z | |
| dc.date.available | 2026-07-07T04:24:05Z | |
| dc.description | Following to the lines drawn in my previous paper about the S=0 relativistic oscillator I build up an oscillatorlike system which can be named as the S=1 Proca oscillator. The Proca field function is obtained in the framework of the Bargmann-Wigner prescription and the interaction is introduced similarly to the S=1/2 Dirac oscillator case regarded by Moshinsky and Szczepaniak. We obtained the intriguing rule of quantization: E = \hbar ω/2 for the parity states (-1)^j and E = \pm \hbar ω(j+1/2) for the parity states -(-1)^j. There are no radial excitations. Finally, I apply the above-mentioned procedure to the case of the two-body relativistic oscillator. | |
| dc.description | ReVTeX file, 7pp., no figures | |
| dc.identifier | https://arxiv.org/abs/hep-th/9801059 | |
| dc.identifier | http://arxiv.org/abs/hep-th/9801059 | |
| dc.identifier | Int.J.Theor.Phys. 39 (2000) 2011-2017 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/55282 | |
| dc.subject | High Energy Physics - Theory | |
| dc.subject | Mathematical Physics | |
| dc.title | More about the S=1 relativistic oscillator | |
| dc.type | text |