Abstract

In this work, we consider a non-quadratic dilaton $\Phi(z)=(\kappa\,z)^{2-\alpha}$ in the context of the static soft wall model to describe the mass spectrum of a wide range of vector mesons from the light up to the heavy sectors. The effect of this non-quadratic approach is translated into non-linear Regge trajectories with the generic form $M^2=a\,(n+b)^\nu$. We apply this sort of fits for the isovector states of $\omega$, $\phi$, $J/\psi$ and $\Upsilon$ mesons and compare with the corresponding holographic duals. We also extend these ideas to the heavy-light sector by using the isovector set of parameters to extrapolate the proper values of $\kappa$ and $\alpha$ through the average constituent mass $\bar{m}$ for each mesonic specie considered. In the same direction, we address the description of possible non-$q\,\bar{q}$ candidates using $\bar{m}$ as a holographic threshold, associated with the structure of the exotic state, to define the values of $\kappa$ and $\alpha$. We study the $\pi_1$ mesons in the light sector, and the $Z_c$, $Y$ and $Z_b$ mesons in the heavy sector as possible exotic vector states. Finally, the RMS error for describing these twenty-seven states with fifteen parameters (four values for $\kappa$ and $\alpha$ respectively and seven values for $\bar{m}$) is $12.61\%$.

Highlights

  • There is no doubt that hadrons are bound states of quarks and gluons, whose interactions are described by quantum chromodynamics (QCD)

  • II we consider four families of isovector mesons with different constituent quarks and we show that these mass spectra agree with a nonlinear Regge trajectory, parametrized by M2 1⁄4 aðn þ bÞν inspired by the parametrization suggested in [18], where a primer interpretation for the exponent ν is to account for the linearity deviation in the radial trajectory

  • It is important to notice that this sort of Regge trajectories is a good description only in the light sector

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Summary

INTRODUCTION

There is no doubt that hadrons are bound states of quarks and gluons, whose interactions are described by quantum chromodynamics (QCD). From the QCD point of view, it is possible to infer the behavior of the potential when the constituent quarks are close or far between them In the former case, the large Q2 limit, the coupling constant is small enough, allowing us to use perturbative techniques to describe the quark interaction by considering the one-gluon exchange only. We explore other kind of dilatons in order to describe hadrons where linear Regge trajectories disagree with experimental data This could be interesting at moment to study, for example, heavy mesons in holographic models, because as it can be seen in literature [22,23,24,25,26,27], AdS/QCD models applied to charmonium or bottomonium spectra are no so good enough to describe them, despite the fact that other observables (as the melting temperature) have the proper qualitative behavior. VI we expose the conclusions and final comments about the present work

NONLINEAR TRAJECTORIES
GEOMETRIC BACKGROUND
MESON MASSES
EXTRAPOLATION TO OTHER MESONIC SPECIES
Heavy-light mesons
Non-qqvector states
Multiquark states
Gluonic excitations
Findings
DISCUSSIONS AND CONCLUSIONS
Full Text
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