Coupling of tṫ over-bar and γγ with a strongly interacting Electroweak Symmetry Breaking Sector

We report the coupling of an external γγ or t(t¯) state to a strongly interacting EWSBS satisfying unitarity. We exploit perturbation theory for those coupling of the external state, whereas the EWSBS is taken as strongly interacting. We use a modified version of the IAM unitarization procedure to m...

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Detalles Bibliográficos
Autor: Delgado López, Rafael
Tipo de recurso: artículo
Fecha de publicación:2017
País:España
Institución:Universidad Complutense de Madrid (UCM)
Repositorio:Docta Complutense
Idioma:inglés
OAI Identifier:oai:docta.ucm.es:20.500.14352/18159
Acceso en línea:https://hdl.handle.net/20.500.14352/18159
Access Level:acceso abierto
Palabra clave:53
Chiral perturbation-theory
Higgs-Boson
Atlas detector
Technicolor theories
Equivalence theorem
Standard model
PP collisions
Mass
Lagrangians
Particle.
Física-Modelos matemáticos
Descripción
Sumario:We report the coupling of an external γγ or t(t¯) state to a strongly interacting EWSBS satisfying unitarity. We exploit perturbation theory for those coupling of the external state, whereas the EWSBS is taken as strongly interacting. We use a modified version of the IAM unitarization procedure to model such a strongly interacting regime. The matrix elements VLVL → V_(L)V_(L), V_(L)V_(L) ↔ hh, hh → hh, V_(L)V_(L) ↔ {γγ, tt¯}, and hh ↔ {γγ, tt¯} are all computed to NLO in perturbation theory with the Nonlinear Effective Field Theory of the EWSBS, within the Equivalence Theorem. This allows us to describe resonances of the electroweak sector that may be found at the LHC and their effect on other channels such as γγ or tt¯ where they may be discovered.