Abstract

We study low-energy nucleon Compton scattering in the framework of baryon chiral perturbation theory (Bχ\chiPT) with pion, nucleon, and Δ\Delta(1232) degrees of freedom, up to and including the next-to-next-to-leading order (NNLO). We include the effects of order p2p^2, p3p^3 and p4/Δp^4/\varDelta, with Δ300\varDelta\approx 300 MeV the Δ\Delta-resonance excitation energy. These are all "predictive" powers in the sense that no unknown low-energy constants enter until at least one order higher (i.e, p4p^4). Estimating the theoretical uncertainty on the basis of natural size for p4p^4 effects, we find that uncertainty of such a NNLO result is comparable to the uncertainty of the present experimental data for low-energy Compton scattering. We find an excellent agreement with the experimental cross section data up to at least the pion-production threshold. Nevertheless, for the proton's magnetic polarizability we obtain a value of (4.0±0.7)×104(4.0\pm 0.7)\times 10^{-4} fm3^3, in significant disagreement with the current PDG value. Unlike the previous χ\chiPT studies of Compton scattering, we perform the calculations in a manifestly Lorentz-covariant fashion, refraining from the heavy-baryon (HB) expansion. The difference between the lowest order HBχ\chiPT and Bχ\chiPT results for polarizabilities is found to be appreciable. We discuss the chiral behavior of proton polarizabilities in both HBχ\chiPT and Bχ\chiPT with the hope to confront it with lattice QCD calculations in a near future. In studying some of the polarized observables, we identify the regime where their naive low-energy expansion begins to break down, thus addressing the forthcoming precision measurements at the HIGS facility.Comment: 24 pages, 9 figures, RevTeX4, revised version published in EPJ

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    Last time updated on 04/12/2019