Elastic electromagnetic form factors of vector mesons
arXiv:1911.05199 · doi:10.1103/PhysRevD.100.114038
Abstract
A symmetry-preserving approach to the two valence-body continuum bound-state problem is used to calculate the elastic electromagnetic form factors of the -meson and subsequently to study the evolution of vector-meson form factors with current-quark mass. To facilitate a range of additional comparisons, form factors are also computed. The analysis reveals that: vector mesons are larger than pseudoscalar mesons; composite vector mesons are non-spherical, with magnetic and quadrupole moments that deviate \% from point-particle values; in many ways, vector-meson properties are as much influenced by emergent mass as those of pseudoscalars; and vector meson electric form factors possess a zero at spacelike momentum transfer. Qualitative similarities between the electric form factors of the and the proton, , are used to argue that the character of emergent mass in the Standard Model can force a zero in . Morover, the existence of a zero in vector meson electric form factors entails that a single-pole vector meson dominance model can only be of limited use in estimating properties of off-shell vector mesons, providing poor guidance for systems in which the Higgs-mechanism of mass generation is dominant.
11 pages, 5 figures, 1 table
References in corpus (20)
- Baryons as relativistic three-quark bound states
- Determination of the Charged Pion Form Factor at Q2=1.60 and 2.45 (GeV/c)2
- Charged pion form factor between Q^2=0.60 and 2.45 GeV^2. II. Determination of, and results for, the pion form factor
- Sketching the Bethe-Salpeter kernel
- Bridging a gap between continuum-QCD and ab initio predictions of hadron observables
- Measurement of gamma gamma* --> pi0 transition form factor at Belle
- Dressed-quark anomalous magnetic moments
- pi- and rho-mesons, and their diquark partners, from a contact interaction
- Vector meson form factors and their quark-mass dependence
- Nucleon electromagnetic form factors from the covariant Faddeev equation
- Charged pion form factor between =0.60 and 2.45 GeV. I. Measurements of the cross section for the H() reaction
- Spectrum of light- and heavy-baryons
- Natural constraints on the gluon-quark vertex
- Spectra of heavy quarkonia in a Bethe-Salpeter-equation approach
- Scaling study of the pion electroproduction cross sections and the pion form factor
- A new method for determining the quark-gluon vertex
- Parton distribution amplitudes of light vector mesons
- Mind the gap
- Light Meson Form Factors at near Physical Masses
- Two Photon Transition Form Factor of Quarkonia