Abstract

In the search for exotic mesons, the GlueX collaboration will soon extract moments of the $\eta\pi^0$ angular distribution. In the perspective of these results, we generalize the formalism of moment extraction to the case in which the two mesons are produced with a linearly polarized beam, and build a model for the reaction $\vec \gamma p \to \eta \pi^0 p$. The model includes resonant $S$-, $P$-, $D$-waves in $\eta\pi^0$, produced by natural exchanges. Moments of the $\eta\pi^0$ angular distribution are computed with and without the $P$-wave, to illustrate the sensitivity to exotic resonances. Although little sensitivity to the $P$-wave is found in moments of even angular momentum, moments of odd angular momentum are proportional to the interference between the $P$-wave and the dominant $S$- and $D$-waves. We also generalize the definition of the beam asymmetry for two mesons photoproduction and show that, when the meson momenta are perpendicular to the reaction plane, the beam asymmetry enhances the sensitivity to the exotic $P$-wave.

Highlights

  • The recent 12 GeV upgrade of continuous electron beam accelerator facility at the Jefferson Lab (JLab) opens a new area in meson spectroscopy studies, especially in addressing the role of gluons in forming exotic hybrid mesons [1]

  • We generalize the definition of the beam asymmetry for two mesons photoproduction and show that, when the meson momenta are perpendicular to the reaction plane, the beam asymmetry enhances the sensitivity to the exotic P wave

  • We find that the maximal sensitivity of the beam asymmetry to the P wave is obtained in the latter case

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Summary

INTRODUCTION

The recent 12 GeV upgrade of continuous electron beam accelerator facility at the Jefferson Lab (JLab) opens a new area in meson spectroscopy studies, especially in addressing the role of gluons in forming exotic hybrid mesons [1]. Exotic contributions, we discuss production of resonant S, P, and D waves in the forward direction, which are produced dominantly by natural exchanges in the t channel [11,12]. 1⁄2lŠ 1⁄4 S, P, D for l 1⁄4 0, 1, 2 is the total spin of the ηπ system To summarize, in this basis for each l, there are 2 × ð2l þ 1Þ complex partial waves for nucleon helicity nonflip and independently 2 × ð2l þ 1Þ amplitudes describing nucleon helicity flip. We assume that the helicity-nonflip amplitudes dominate and set the helicityflip amplitudes to zero This is not restrictive, as the target is not polarized in GlueX, and the measured intensities are not sensitive to the details of the nucleon helicity structure. Observables (moments and beam asymmetries) extracted in the helicity frame can be computed in the s-channel frame.

MOMENTS
General definition
Beam asymmetry along the y axis
Illustration of beam asymmetries
CONCLUSIONS
Full Text
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