Compositeness Condition
| dc.creator | Akama, Keiichi | |
| dc.date | 1997-06-21 | |
| dc.date.accessioned | 2026-07-07T04:01:58Z | |
| dc.date.available | 2026-07-07T04:01:58Z | |
| dc.description | By solving the compositeness condition, under which the Yukawa-type model coincides the NJL type model, we obtain the expressions for the effective coupling constants in terms of the compositeness scale at the next-to-leading order in 1/N. In the NJL model with a scalar composite, the next to leading contributions are too large for N_c=3. In the induced gauge theory with abelian gauge symmetry, the correction term is reasonably suppressed, while in the non-abelian gauge theory the corrections are suppressed only when it is asymptotically non-free. | |
| dc.description | 6 pages, revtex, Talk given at Shizuoka Workshop on Masses and Mixing of Quarks and Leptons, Shizuoka, Japan, March 1997. To be published in Proceedings | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9706442 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9706442 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/47045 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Compositeness Condition | |
| dc.type | text |