Abstract

We discuss cross-link relations between the $\ensuremath{\pi}$ and $\ensuremath{\rho}$-meson channels emerging from two different descriptions of the QCD vacuum: instanton physics and QCD sum rules with nonlocal condensates (NLCs). We derive in both schemes an intriguing linear relation between the $\ensuremath{\pi}$ and the ${\ensuremath{\rho}}^{\ensuremath{\parallel}}$-meson distribution amplitudes in terms of their conformal coefficients and work out the specific impact of the scalar NLC in these two channels. Using a simple model with Gaussian decay of the scalar NLC, we are able to relate it to the moments of the pion nonsinglet parton distribution function measurable in experiment---a highly nontrivial result. The implications for the pion and the ${\ensuremath{\rho}}^{\ensuremath{\parallel}}$-meson distribution amplitudes entailed by the obtained cross-link relations are outlined in terms of two generic scenarios.

Highlights

  • Polyakov and Son [1] have employed the instanton approach in combination with dispersion relations for the two-pion distribution amplitude (DA) [2] to obtain model-independent relations for the ratio að2ρÞ=að2πÞ

  • We discuss cross-link relations between the π and ρ-meson channels emerging from two different descriptions of the QCD vacuum: instanton physics and QCD sum rules with nonlocal condensates (NLCs)

  • We derive in both schemes an intriguing linear relation between the π and the ρk-meson distribution amplitudes in terms of their conformal coefficients and work out the specific impact of the scalar NLC in these two channels

Read more

Summary

INTRODUCTION

Polyakov and Son [1] have employed the instanton approach in combination with dispersion relations for the two-pion distribution amplitude (DA) [2] to obtain model-independent relations for the ratio að2ρÞ=að2πÞ. Let us emphasize the good correspondence in (i) and (ii) between the segments of að2πÞ and að2ρÞ derived from NLC-SR This circumstance makes it tempting to derive a relation similar to Eq (3) within the NLC-SR approach for the pion [6,20] and the ρk meson [19,20,21]. The dependence of the scalar NLC ΦSðx; M2Þ on the Borel scale M2 and the quark virtuality λ2q 1⁄4 0.4 GeV2 is given graphically, making use of the simplest Gaussian model for the QCD vacuum from Refs. The notation 1⁄4sr means that one should take the average of the rhs over M2 within the stability window in the Borel parameter, i.e., 0.55 GeV2 1⁄4 M2− < M2 ≲ M2þ 1⁄4 1.1 GeV2; in order to obtain a certain numerical value of the lhs

CONNECTION BETWEEN SCALAR NLC AND PION PDF
Conformal expansion beyond second order
IMPLICATIONS FOR THE ρk-MESON AND PION DA
CONCLUSIONS
18 Δ Δ2 fθðx
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call