Resumen
The present notes prepare the counting of 'oscillatory modes of N fl = 3 light quarks', - u, d, s -, using the SU (2 Nfl = 6) × SO3 (L) broken symmetry classification, extended to the harmonic oscillator symmetry of 3 paired oscillator modes. L = ΣNfl n =1 Ln stands for the space rotation group generated by the sum of the 3 individual angular momenta of quarks in their c.m. system. The motivation arises from modeling the yields of hadrons in heavy ion collisions at RHIC and LHC, necessitating at the respective highest c.m. energies per nucleon pairs an increase of heavy hadron resonances relative to e.g. SPS energies, whence the included hadrons are treated as a noninteracting gas.
| Idioma original | Inglés |
|---|---|
| Número de artículo | 00090 |
| Publicación | EPJ Web of Conferences |
| Volumen | 71 |
| DOI | |
| Estado | Publicada - 2014 |
| Publicado de forma externa | Sí |
| Evento | 2nd International Conference on New Frontiers in Physics, ICNFP 2013 - Kolymbari, Crete, Grecia Duración: 28 ago 2013 → 5 sept 2013 |
Huella
Profundice en los temas de investigación de 'Oscillatory modes of quarks in baryons for 3 quark flavors u,d,s: Tuning to harmonic numbers of oscimodes of baryons'. En conjunto forman una huella única.Citar esto
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