Abstract

We investigate the axial-vector nucleon-to-delta transition form factors in the framework of relativistic baryon chiral perturbation theory at the one-loop order using the complex-mass renormalization scheme. We determine the available six free parameters by fitting to an empirical parametrization of the form factors obtained from the BNL neutrino bubble chamber experiments. A unique feature of our calculation is the prediction of a non-vanishing form factor $C_3^A(Q^2)$. Moreover, our results show a surprising sensitivity to the coupling constant $\texttt{g}_1$ of the leading-order Lagrangian ${\cal L}^{(1)}_{\pi \Delta}$.

Highlights

  • The Δð1232Þ resonance is the first and best-established excitation of the nucleon [1]

  • We investigate the axial-vector nucleon-to-delta transition form factors in the framework of relativistic baryon chiral perturbation theory at the one-loop order using the complex-mass renormalization scheme

  • We determine the available six free parameters by fitting to an empirical parametrization of the form factors obtained from the BNL neutrino bubble chamber experiments

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Summary

INTRODUCTION

The Δð1232Þ resonance is the first and best-established excitation of the nucleon [1]. While there is a substantial amount of empirical information on the electromagnetic (vector) nucleon-to-delta transition [2,3,4,5,6,7,8,9,10,11,12,13,14,15] [38] that form factors of unstable particles should be determined from the renormalized three-point function at the complex pole [23] to the electromagnetic nucleon-to-Δ resonance transition to third chiral order in manifestly Lorentzinvariant chiral effective field theory.

Weak pion production
Definition of the axial-vector transition form factors
Pion-nucleon-delta transition form factor
EFFECTIVE LAGRANGIAN AND POWER COUNTING
RESULTS
COMPARISON WITH OTHER WORK
SUMMARY
Full Text
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