Abstract

In this paper, we study the pion leading-twist distribution amplitude (DA) ${\ensuremath{\phi}}_{2;\ensuremath{\pi}}(x,\ensuremath{\mu})$ by improving the traditional light-cone harmonic oscillator model within the reconstruction of the function ${\ensuremath{\varphi}}_{2;\ensuremath{\pi}}(x)$. In order to constrain the model parameters, we calculate its moments $⟨{\ensuremath{\xi}}^{n}{⟩}_{2;\ensuremath{\pi}}{|}_{\ensuremath{\mu}}$ in the framework of the QCD background field theory sum rule up to tenth order. Considering the fact that the sum rule of the zeroth moment $⟨{\ensuremath{\xi}}^{0}{⟩}_{2;\ensuremath{\pi}}{|}_{\ensuremath{\mu}}$ cannot be normalized, we suggest a more reasonable sum rule formula for $⟨{\ensuremath{\xi}}^{n}{⟩}_{2;\ensuremath{\pi}}{|}_{\ensuremath{\mu}}$. Then, we obtain the values of $⟨{\ensuremath{\xi}}^{n}{⟩}_{2;\ensuremath{\pi}}{|}_{{\ensuremath{\mu}}_{0}}$ with $n=(2,4,6,8,10)$ at the initial scale ${\ensuremath{\mu}}_{0}=1\text{ }\text{ }\mathrm{GeV}$. The first two moments are $⟨{\ensuremath{\xi}}^{2}{⟩}_{2;\ensuremath{\pi}}{|}_{{\ensuremath{\mu}}_{0}}=0.271\ifmmode\pm\else\textpm\fi{}0.013$ and $⟨{\ensuremath{\xi}}^{4}{⟩}_{2;\ensuremath{\pi}}{|}_{{\ensuremath{\mu}}_{0}}=0.138\ifmmode\pm\else\textpm\fi{}0.010$, and the corresponding Gegenbauer moments are ${a}_{2}^{2;\ensuremath{\pi}}({\ensuremath{\mu}}_{0})=0.206\ifmmode\pm\else\textpm\fi{}0.038$ and ${a}_{4}^{2;\ensuremath{\pi}}({\ensuremath{\mu}}_{0})=0.047\ifmmode\pm\else\textpm\fi{}0.011$, respectively. After fitting the moments $⟨{\ensuremath{\xi}}^{n}{⟩}_{2;\ensuremath{\pi}}{|}_{\ensuremath{\mu}}$, we obtain the appropriate model parameters by using the least squares method. The resultant behavior for the twist-2 pion DA is closer to the AdS/QCD and lattice results, but narrower than that obtained using the Dyson-Schwinger equation. Furthermore, we calculate the pion-photon transition form factors (TFFs) and $B\ensuremath{\rightarrow}\ensuremath{\pi}$ TFFs within the light-cone sum rule approach, which conform with experimental and theoretical results.

Highlights

  • Light meson light-cone distribution amplitudes (DAs) are universal nonperturbative objects, which describe the momentum fraction distributions of partons in a meson for a particular Fock state

  • In the standard treatment of exclusive processes in QCD proposed by Brodsky and Lepage [1], cross sections are arranged according to different twist structures of meson DAs, in which the leading-twist DA contribution usually dominates due to the fact that the contributions

  • We study the pionic leading-twist DA φ2;πðx; μÞ based on the improved light-cone harmonic oscillator (LCHO) model

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Summary

INTRODUCTION

Light meson light-cone distribution amplitudes (DAs) are universal nonperturbative objects, which describe the momentum fraction distributions of partons in a meson for a particular Fock state. People usually adopt the truncated form involving only the first few terms in the Gegenbauer expansion series as an approximate form of φ2;πðx; μÞ Those Gegenbauer moments can be calculated directly via some nonperturbative methods, such as QCD sum rules [4,5,6,7,8,9] or lattice gauge theory [10,11,12,13]. Due to the incompleteness of our sum rules calculation, the deviation of hξ0i2;πjμ from the normalization must be considered This motivates us to recalculate the moments of the pionic leading-twist DA with QCD sum rules.

THEORETICAL FRAMEWORK
Basic input parameters
Model parameters of the pionic leading-twist DA and applications
Method
Findings
SUMMARY
Full Text
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