γ(∗) + ()⁢/+ → ()/− helicity amplitudes and transition form factors

We recently reported new results on the (*)+⁡(940)⁢1/2+→Δ⁡(1700)⁢ 3/2− transition form factors using a symmetry-preserving treatment of a vector ⊗vector contact interaction (SCI) within a coupled formalism based on the Dyson-Schwinger, Bethe-Salpeter, and Faddeev equations. In this work, we extend o...

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Detalles Bibliográficos
Autores: Albino, L., Paredes Torres, Gustavo, Raya, Khépani, Bashir, Adnan, Segovia González, Jorge
Tipo de recurso: artículo
Fecha de publicación:2025
País:España
Institución:Universidad de Huelva (UHU)
Repositorio:Arias Montano. Repositorio Institucional de la Universidad de Huelva
Idioma:inglés
OAI Identifier:oai:ariasmontano.uhu.es:10272/27367
Acceso en línea:https://hdl.handle.net/10272/27367
Access Level:acceso abierto
Palabra clave:2208.07 Física de Partículas
2212 Física Teórica
Descripción
Sumario:We recently reported new results on the (*)+⁡(940)⁢1/2+→Δ⁡(1700)⁢ 3/2− transition form factors using a symmetry-preserving treatment of a vector ⊗vector contact interaction (SCI) within a coupled formalism based on the Dyson-Schwinger, Bethe-Salpeter, and Faddeev equations. In this work, we extend our investigation to the (*)+⁡(940)⁢1/2+ →⁡(1520)⁢3/2− transition. Our computed transition form factors show reasonable agreement with experimental data at large photon virtualities. However, deviations emerge at low 2, where experimental results exhibit a sharper variation than theoretical predictions. This discrepancy is expected, as these continuum QCD analyses account only for the quark-core of baryons, while low photon virtualities are dominated by meson cloud effects. We anticipate that these analytical predictions, based on the simplified SCI framework, will serve as a valuable benchmark for more refined studies and QCD-based truncations that incorporate quark angular momentum and the contributions of scalar and vector diquarks.