English

Pion model with the Nakanishi Integral Representations

High Energy Physics - Phenomenology 2022-02-24 v2 Nuclear Theory

Abstract

In the present work, we describe a model for the pion based on an analytic expression for the Bethe-Salpeter (BSA) amplitude, combined with some ingredients from Lattice QCD calculations. The running quark mass function M(p2)M (p^2), used here, reproduces well the results of Lattice QCD calculations. The analytical form of the running quark mass function contains a single time-like pole, which implies in time-like poles of the dressed quark propagator. Such a form allows to build the weight functions, Gi(γ,z)G_i(\gamma,z), for the Nakanishi integral representation of each scalar function, χi(k,p)\chi_{i}(k,p), appearing in the decomposition of the Bethe-Salpeter amplitude in terms of Dirac operators, Such scalar amplitudes can also be used to obtain the pion valence light-front wave function.

Cite

@article{arxiv.2202.10959,
  title  = {Pion model with the Nakanishi Integral Representations},
  author = {R. M. Moita and J. P. B. C. de Melo and T. Frederico and W. de Paula},
  journal= {arXiv preprint arXiv:2202.10959},
  year   = {2022}
}

Comments

6 pages, 5 figures (eps). Contribuition to the "19 th International Conference on Hadron Spectroscopy and Structure (HADRON 2021)", Mexico, 2021 To appear "Suplemento de la Revista Mexicana de Fisica"

R2 v1 2026-06-24T09:49:47.987Z