Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry
We consider the generalization of the meson bootstrap scheme to SW̄(3) symmetry, assigning the spin zero mesons to the (3,3*) (3*,3) representation. We find that the leading Regge trajectory is an SW̄(3) singlet and identify it with the Pomeranchuk trajectory. In addition we observe that the self-co...
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1966
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paper:paper_0031899X_v145_n4_p1154_Munczek2023-06-08T14:57:45Z Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry Munczek, Hermán Jaime Pignotti, Alberto Virasoro, Miguel Angel José We consider the generalization of the meson bootstrap scheme to SW̄(3) symmetry, assigning the spin zero mesons to the (3,3*) (3*,3) representation. We find that the leading Regge trajectory is an SW̄(3) singlet and identify it with the Pomeranchuk trajectory. In addition we observe that the self-consistent solution includes the vector and axial vector mesons in the (1,8) (8,1) and the spin 2 mesons in the (3,3*) (3*,3) representation. Thus we predict the existence of a tenth JP=2+ meson. We suggest that the missing meson is the Pomeranchuk particle and that it should be found at an energy considerably smaller than the 2+ nonet mass. © 1966 The American Physical Society. Fil:Munczek, H. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Pignotti, A. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Virasoro, M.A. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. 1966 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_0031899X_v145_n4_p1154_Munczek http://hdl.handle.net/20.500.12110/paper_0031899X_v145_n4_p1154_Munczek |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
repository_str |
R-134 |
collection |
Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
description |
We consider the generalization of the meson bootstrap scheme to SW̄(3) symmetry, assigning the spin zero mesons to the (3,3*) (3*,3) representation. We find that the leading Regge trajectory is an SW̄(3) singlet and identify it with the Pomeranchuk trajectory. In addition we observe that the self-consistent solution includes the vector and axial vector mesons in the (1,8) (8,1) and the spin 2 mesons in the (3,3*) (3*,3) representation. Thus we predict the existence of a tenth JP=2+ meson. We suggest that the missing meson is the Pomeranchuk particle and that it should be found at an energy considerably smaller than the 2+ nonet mass. © 1966 The American Physical Society. |
author |
Munczek, Hermán Jaime Pignotti, Alberto Virasoro, Miguel Angel José |
spellingShingle |
Munczek, Hermán Jaime Pignotti, Alberto Virasoro, Miguel Angel José Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry |
author_facet |
Munczek, Hermán Jaime Pignotti, Alberto Virasoro, Miguel Angel José |
author_sort |
Munczek, Hermán Jaime |
title |
Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry |
title_short |
Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry |
title_full |
Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry |
title_fullStr |
Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry |
title_full_unstemmed |
Tenth JP=2+ meson as a dynamical consequence of SW̄(3) symmetry |
title_sort |
tenth jp=2+ meson as a dynamical consequence of sw̄(3) symmetry |
publishDate |
1966 |
url |
https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_0031899X_v145_n4_p1154_Munczek http://hdl.handle.net/20.500.12110/paper_0031899X_v145_n4_p1154_Munczek |
work_keys_str_mv |
AT munczekhermanjaime tenthjp2mesonasadynamicalconsequenceofsw3symmetry AT pignottialberto tenthjp2mesonasadynamicalconsequenceofsw3symmetry AT virasoromiguelangeljose tenthjp2mesonasadynamicalconsequenceofsw3symmetry |
_version_ |
1768544540276293632 |