Abstract

In this work, we argue that the observed differences in the value of the vector coupling constant extracted from the decays $\ensuremath{\rho}\ensuremath{\rightarrow}\ensuremath{\pi}\ensuremath{\pi}$ (${g}_{\ensuremath{\rho}}=6.0$), $\ensuremath{\rho}\ensuremath{\rightarrow}{l}^{+}{l}^{\ensuremath{-}}$ (${g}_{\ensuremath{\rho}}=5.0$) and $\ensuremath{\omega}\ensuremath{\rightarrow}{l}^{+}{l}^{\ensuremath{-}}$ (${g}_{\ensuremath{\rho}}=5.7$), where $l=e$, $\ensuremath{\mu}$, are an indication of the important role played by the $1/{N}_{c}$ corrections in the description of these processes. We show that an emission of a photon by charged meson loops in the ${\ensuremath{\rho}}^{0},\ensuremath{\omega},\ensuremath{\phi}\ensuremath{\rightarrow}\ensuremath{\gamma}$ transitions is a key process that allows to describe above vector meson decays into two leptons with a single value ${g}_{\ensuremath{\rho}}=6.0$. Our result supports the idea of universality of neutral vector mesons and clarifies the role of accounting of $1/{N}_{c}$ corrections to its fulfilment.

Highlights

  • It is well known that the hypothesis of vector-meson dominance (VMD) [1,2] possesses one to compute the lepton-pair decay rate of the neutral vector meson V 1⁄4 ρ0; ω; φ in terms of the vector-meson coupling constant fV appearing in a current-field identity Jem 1⁄4 P m2V V

  • We argue that the observed differences in the value of the vector coupling constant extracted from the decays ρ → ππ, ρ → lþl− and ω → lþl−, where l 1⁄4 e, μ, are an indication of the important role played by the 1=Nc corrections in the description of these processes

  • We show that an emission of a photon by charged meson loops in the ρ0; ω; φ → γ transitions is a key process that allows to describe above vector meson decays into two leptons with a single value gρ 1⁄4 6.0

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Summary

INTRODUCTION

It is well known that the hypothesis of vector-meson dominance (VMD) [1,2] possesses one to compute the lepton-pair decay rate of the neutral vector meson V 1⁄4 ρ0; ω; φ in terms of the vector-meson coupling constant fV appearing in a current-field identity Jem 1⁄4 P m2V V. Current experimental data on V → lþl− decay widths [3] allow to determine from (1) the phenomenological values of these constants. From the set of all 1= Nc order one-loop amplitudes contributing to V → lþl− decay one may exclude diagrams of the vector meson self-energy type. These diagrams were considered in [16] with the conclusion that the coupling constant fV remains unaltered. As we will show below, in the case of V → lþl− decays, meson loops V → ΦΦ → γ lead to the correct description of two-lepton decay modes with the original value of the coupling constant gρ 1⁄4 6.0.

DYNAMIC SYMMETRIES AND UNIVERSALITY
LARGE Nc LIMIT AND UNIVERSALITY
SUð3Þ VIOLATION
I2ðm2uÞ
CONCLUSIONS
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