Abstract

We use the energy–momentum tensor (EMT) current to compute the EMT form factors of the nucleon in the framework of the light cone QCD sum rule formalism. In the calculations, we employ the most general form of the nucleon’s interpolating field and use the distribution amplitudes (DAs) of the nucleon with two sets of the numerical values of the main input parameters entering the expressions of the DAs. The directly obtained results from the sum rules for the form factors are reliable at Q^2ge 1 GeV^2 : to extrapolate the results to include the zero momentum transfer squared with the aim of estimation of the related static physical quantities, we use some fit functions for the form factors. The numerical computations show that the energy–momentum tensor form factors of the nucleon can be well fitted to the multipole fit form. We compare the results obtained for the form factors at Q^2=0 with the existing theoretical predictions as well as experimental data on the gravitational form factor d_1^q(0). For the form factors M_2^q (0) and J^q(0) a consistency among the theoretical predictions is seen within the errors: our results are nicely consistent with the Lattice QCD and chiral perturbation theory predictions. However, there are large discrepancies among the theoretical predictions on d_1^q(0). Nevertheless, our prediction is in accord with the JLab data as well as with the results of the Lattice QCD, chiral perturbation theory and KM15-fit. Our fit functions well define most of the JLab data in the interval Q^2in [0,0.4] GeV^2 , while the Lattice results suffer from large uncertainties in this region. As a by-product, some mechanical properties of the nucleon like the pressure and energy density at the center of nucleon as well as its mechanical radius are also calculated and their results are compared with other existing theoretical predictions.

Highlights

  • The explicit expressions of the energy–momentum tensor form factors (EMTFFs) are moved to Appendix B

  • The central values of the form factors at Q2 = 0 obtained via two sets of distribution amplitudes differ slightly from each other but they are consistent within the presented errors

  • The EMTFFs are sources of information on the fractions of the momenta carried by the quarks and gluons as ingredients of the nucleon

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Summary

Motivation

Understanding of the inner structures of the nucleons based on the quarks and gluons degrees of freedom is one of the most prominent research subjects of the hadron physics. [13] Hagler et al presented a exhaustive study of the lowest moments of nucleon GPDs in 2 + 1 Lattice QCD by the help of domain wall valence quarks and refined staggered sea quarks without including the disconnected diagrams They performed extrapolations of their results based on different chiral effective field theory schemes at re-normalization scale of μ2 = 4 GeV2. [22], Dorati et al evaluated the basic properties related to the structures of baryons at low energies, by the help of the method of the covariant chiral perturbation theory in the baryon sector at leading-one-loop order They investigated the quark-mass dependence of the isoscalar moments in the forward limit and estimated the contributions of quarks to the total spin of the nucleon at re-normalization scale of μ = 2 GeV. The explicit expressions of the EMTFFs are moved to Appendix B

Formalism
Numerical results
Mechanical properties of nucleon
Summary and concluding remarks
Full Text
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