Abstract

Abstract We study the elastic and radiative π+p scattering within a full dynamical model which incorporates the finite width effects of the Δ++. The scattering amplitudes are invariant under contact transformations of the spin 3/2 field and gauge-invariance is fulfilled for the radiative case. The pole parameters of the Δ++ obtained from the elastic cross section are mΔ=(1211.2±0.4) MeV and ΓΔ=(88.2±0.4) MeV. From a fit to the most sensitive observables in radiative π+p scattering, we obtain μΔ=(6.14±0.51)e/2mp for the magnetic dipole moment of the Δ++.

Highlights

  • The description of resonances in particle physics has gotten a renewed interest with the advent of precise measurements of the Z0 gauge boson properties at LEP [1]

  • We study the elastic and radiative π+p scattering within a full dynamical model which incorporates the finite width effects of the ∆++

  • The model, to be described below, reproduces very well the total and differential cross sections for elastic π+p scattering close to the resonance region. This model provides an amplitude for radiative π+p scattering that satisfies electromagnetic gauge invariance when finite width effects of the ∆++ resonance are taken into account

Read more

Summary

Introduction

The description of resonances in particle physics has gotten a renewed interest with the advent of precise measurements of the Z0 gauge boson properties at LEP [1]. We study the elastic and radiative π+p scattering within a full dynamical model which incorporates the finite width effects of the ∆++. The aim of the present Letter is to determine the magnetic dipole moment (MDM) of the ∆++ resonance by using a full dynamical model which consistently describes elastic and radiative π+p scattering data.

Results
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.