Abstract

Taking into account only the quark part of the energy-momentum tensor, the gravitational form-factors of the $ \pi $ and $ K $ mesons are calculated within the light-cone sum rules method using the distribution amplitudes of these pseudoscalar mesons. The $ Q^2 $-dependence of the relevant form-factors are obtained. Moreover, the mean square mass radii of $ \pi $ and $ K $ mesons are calculated and we find that $ \sqrt{\langle r_{\pi}^2 \rangle} = 0.31 {\rm\ fm} $ and $ \sqrt{\langle r_{K}^2 \rangle} = 0.24 {\rm\ fm} $, respectively. We compare our results for gravitational form-factors with the existing literature results. We obtain that our results on $ \sqrt{\langle r_\pi^2 \rangle} $ are in good agreement with the predictions of NJL model, AdS/QCD model, and other models as well as with the existing experimental data.

Highlights

  • During the last years, the energy-momentum tensor (EMT) has become one of the popular research objects for understanding better the structure of hadrons [1,2]

  • We study the gravitational formfactors (GFFs) of the ρ, π, and K mesons within the light-cone sum rules (LCSR)

  • We studied the GFFs appearing in the decompositions of the quark part of the energymomentum tensor for ρ, π, and K mesons within the light-cone QCD sum rules approach

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Summary

INTRODUCTION

The energy-momentum tensor (EMT) has become one of the popular research objects for understanding better the structure of hadrons [1,2]. The GFFs of the ρ meson were studied within the lightcone constituent quark model in [12]. The GFFs of the π meson were studied in the chiral limit of a hard-wall AdS/QCD [17], in the NJL model [16], by using the generalized distribution amplitudes [18], in the lattice QCD [19], and in hard electroproduction processes [20]. We study the GFFs of the ρ, π, and K mesons within the light-cone sum rules (LCSR). The LCSR method is powerful in that it provides consistently taking into account the hard and soft contributions to exclusive processes and establishes a bridge to connect the distribution amplitudes (DAs) of hadrons and formfactors. In the LCSR method, the operator product expansion (OPE) is performed over twist rather than

Published by the American Physical Society
In addition conditions
JAλ and q μν and by using the
Gαβ εαβμνGμν is the dual gluon field strength tensor
Findings
CONCLUSION
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