Abstract:Abstract. The interference effect between leptonic radiative corrections and hadronic polarization functions is calculated via optical theorem for µ−pair production in vicinity of narrow resonances. Within seven most dominant exclusive channels of the production cross section σ h (e + e − → hadrons) one achieves high acuracy which is necessary for the comparison with experiments. The result is compared with KLOE and KLOE2 experiments for µ − µ + and µ − µ + γ productions at φ and ω/ρ meson energy.
“…In this figure we compare the norm square and compare with world averaged experimental data for F . The averaged experimental based on data of BABAR, BESS, CMD/SND and KLOE experiments [1] were fitted as described in [82], noting there is negligibly small experimental error 0.5% on the ρ meson peak. Within used approximation the derivation of desired dispersion relation (4.8) is quite straightforward, albeit a bit lengthy and it is delegated into the Appendix C of this work.…”
The electromagnetic form factor of the pion is calculated within the use of functional formalism. We develop Integral Representation for the minimal set of Standard Model Green's functions and derive the dispersion relation for the form factor in two flavor QCD isospin limit mu = m d . We use dressed quark propagator as obtained form the gap equation in Minkowski space and derive the approximate dispersion relation for the form factor. We evaluate the form factor for the spacelike as well as for the timelike momentum in presented formalism for the first time. A new Nakanishi like form of integral representation is proved on the base of vector Bethe-Salpeter equation for the quarkphoton vector with ladder-rainbow kernel. The Gauge Technique turns to be a part of the entire structure of the vertex. In analytic approach presented here, it is shown that the large amount of ρ meson peak in the cross section e + e − → π + π − is governed by the gauge invariance of QED/QCD, i.e. by Gauge Technique constructed quark-photon vertex. This approximation naturally explains the broad shape of the ρ meson peak.
“…In this figure we compare the norm square and compare with world averaged experimental data for F . The averaged experimental based on data of BABAR, BESS, CMD/SND and KLOE experiments [1] were fitted as described in [82], noting there is negligibly small experimental error 0.5% on the ρ meson peak. Within used approximation the derivation of desired dispersion relation (4.8) is quite straightforward, albeit a bit lengthy and it is delegated into the Appendix C of this work.…”
The electromagnetic form factor of the pion is calculated within the use of functional formalism. We develop Integral Representation for the minimal set of Standard Model Green's functions and derive the dispersion relation for the form factor in two flavor QCD isospin limit mu = m d . We use dressed quark propagator as obtained form the gap equation in Minkowski space and derive the approximate dispersion relation for the form factor. We evaluate the form factor for the spacelike as well as for the timelike momentum in presented formalism for the first time. A new Nakanishi like form of integral representation is proved on the base of vector Bethe-Salpeter equation for the quarkphoton vector with ladder-rainbow kernel. The Gauge Technique turns to be a part of the entire structure of the vertex. In analytic approach presented here, it is shown that the large amount of ρ meson peak in the cross section e + e − → π + π − is governed by the gauge invariance of QED/QCD, i.e. by Gauge Technique constructed quark-photon vertex. This approximation naturally explains the broad shape of the ρ meson peak.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.