Abstract

The issue of the contribution of zero-modes to the light-front projection of the electromagnetic current of phenomenological models of vector particles vertices is addressed in the Drell–Yan frame. Our analytical model of the Bethe–Salpeter amplitude of a spin-1 fermion–antifermion composite state gives a physically motivated light-front wave function symmetric by the exchange of the fermion and antifermion, as in the ρ-meson case. We found that among the four independent matrix elements of the plus component in the light-front helicity basis only the 0→0 one carries zero-mode contributions. Our derivation generalizes to symmetric models, important for applications, the above conclusion found for a simplified non-symmetrical form of the spin-1 Bethe–Salpeter amplitude with photon–fermion point-like coupling and also for a smeared fermion–photon vertex model.

Highlights

  • The issue of the contribution of zero-modes to the light-front projection of the electromagnetic current of phenomenological models of vector particles vertices is addressed in the Drell-Yan frame

  • We show analytically that zero-mode contributions appearing in the matrix elements of the spin-1 electromagnetic current are canceled in the computation of form factors with the prescription suggested by Ref. [27]

  • We compute: i) the direct term with γμ vertices from the initial and final states of the vector particle; ii) the cross term with γμ and derivative coupling; iii) the direct term with two derivative couplings. This strategy simplifies the separation of zero-mode contributions present in the different terms of the matrix elements of the electromagnetic current and electromagnetic form factors of the composite vector state

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Summary

Introduction

The issue of the contribution of zero-modes to the light-front projection of the electromagnetic current of phenomenological models of vector particles vertices is addressed in the Drell-Yan frame. We show analytically that zero-mode contributions appearing in the matrix elements of the spin-1 electromagnetic current are canceled in the computation of form factors with the prescription suggested by Ref.

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