Abstract

We investigate nonlinear extensions of the holographic soft wall model proposed by Karch et al. [Phys. Rev. D 74, 015005 (2006)] with a positive quadratic dilaton. We consider a Higgs potential for the tachyonic field that brings a more natural realization of chiral symmetry breaking in the infrared regime. Utilizing the $\mathrm{AdS}/\mathrm{CFT}$ dictionary and holographic renormalization, we find the chiral condensate as a function of the quark mass. The nonlinearity of the Higgs potential leads to a nonlinear relation between the chiral condensate and the quark mass. Solving the effective Schr\"odinger equations for the field perturbations, we estimate meson masses and decay constants and evaluate their dependence on the quark mass. In the axial and pseudoscalar sector we find an interesting behavior for the decay constants as the quark mass increases. We also investigate the effect of a five-dimensional running mass for the tachyonic field. We conclude that nonlinear soft wall models with a Higgs potential for the tachyon and a positive quadratic dilaton do not provide spontaneous symmetry breaking in the chiral limit.

Highlights

  • The dynamical breaking of chiral symmetry in quantum chromodynamics (QCD) is a fascinating phenomenon that occurs in the strongly coupled regime

  • We conclude that nonlinear soft wall models with a Higgs potential for the tachyon and a positive quadratic dilaton do not provide spontaneous symmetry breaking in the chiral limit

  • In this work we investigated a nonlinear realization for chiral symmetry breaking in soft wall models based on a Higgs potential

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Summary

INTRODUCTION

The dynamical breaking of chiral symmetry in quantum chromodynamics (QCD) is a fascinating phenomenon that occurs in the strongly coupled (nonperturbative) regime. The chiral condensate hqqi is proportional to the quark mass mq just as a consequence of the linearity of the tachyonic field equation This implies, in particular, that taking the chiral limit mq → 0 in the soft wall model does not lead to spontaneous chiral symmetry breaking (the chiral condensate vanishes). In this work we perform a systematic analysis of the background and field perturbations for nonlinear soft wall models based on a positive quadratic dilaton Φ and a Higgs potential for the tachyonic field X. Our approach was partially inspired by the holographic QCD model of [10], where chiral symmetry breaking maps to tachyon condensation in string theory. Appendix B briefly reviews the holographic model of [11], while Appendix C describes some complementary numerical results

HARD AND SOFT WALL MODELS FOR CHIRAL SYMMETRY BREAKING
NONLINEAR SOFT WALL MODELS
Numerical solution
Holographic renormalization and the chiral condensate
Counterterms and covariant subtraction
Spectrum of the vector sector
Spectrum of the scalar sector
Spectrum of the axial-vector sector
Spectrum of the pseudoscalar sector
Decay constants
NONLINEAR SOFT WALL MODELS WITH RUNNING MASS
DISCUSSION AND CONCLUSIONS
Scalar sector

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