Intrinsic Parity of the $(j,0)\oplus(0,j)$ Mesons
| dc.creator | Ahluwalia, D. V. | |
| dc.date | 1992-11-13 | |
| dc.date.accessioned | 2026-07-07T03:55:46Z | |
| dc.date.available | 2026-07-07T03:55:46Z | |
| dc.description | Contrary to the usual belief, by carefully examining the operation of parity transformation on the $(1,0)\oplus(0,1)$ mesons in the generalized canonical representation, we establish that the $(j,0)\oplus(0,j)$ meson-antimeson pair have {\it opposite} intrinsic parity. This opens up the possibility that while the particles without an internal structure may utilize one representation of the Lorentz group, phenomenologies of composite particles may exploit a different representation. As such (perhaps, only some of) the meson structures beyond the standard $q\,\overline {Q}$ may exploit the $(j,0)\oplus(0,j)$ generalized canonical representation of the Lorentz group -- this would result in a meson and the associated antimeson to manifest themselves in {\it different} partial waves. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% CONSTRUCTIVE COMMENTS WELCOME, AS ALWAYS D. V. A. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% | |
| dc.description | 8 pages, LA-UR-92-3726, Latex | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9211245 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9211245 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/44680 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | Nuclear Theory | |
| dc.title | Intrinsic Parity of the $(j,0)\oplus(0,j)$ Mesons | |
| dc.type | text |