Limitations of the heavy-baryon expansion as revealed by a pion-mass dispersion relation

Abstract

The chiral expansion of nucleon properties such as mass, magnetic moment, and magnetic polarizability are investigated in the framework of chiral perturbation theory, with and without the heavy-baryon expansion. The analysis makes use of a pion-mass dispersion relation, which is shown to hold in both frameworks. The dispersion relation allows an ultraviolet cutoff to be implemented without compromising the symmetries. After renormalization, the leading-order heavy-baryon loops demonstrate a stronger dependence on the cutoff scale, which results in weakened convergence of the expansion. This conclusion is tested against the recent results of lattice quantum chromodynamics simulations for nucleon mass and isovector magnetic moment. In the case of the polarizability, the situation is even more dramatic as the heavy-baryon expansion is unable to reproduce large soft contributions to this quantity. Clearly, the heavy-baryon expansion is not suitable for every quantity.

Accepted for publication in EPJ C. Made changes based on referee comments: clarifying sentences to conclusion 1. of Section IV, beginning of Section V, and new footnote in Section VI, page 8. Added more detailed explanation in paragraph 4 of Section III. Added citations of Phys.Rev. D60, 034014, and Phys.Lett. B716, 338

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Cited by in corpus (5)

• Nucleon Polarizabilities: from Compton Scattering to Hydrogen Atom
• Chiral perturbation theory of muonic hydrogen Lamb shift: polarizability contribution
• On the convergence of the chiral expansion for the baryon ground-state masses
• Finite-volume and partial quenching effects in the magnetic polarizability of the neutron
• Generalized polarizabilities of the nucleon in baryon chiral perturbation theory