We study low-energy nucleon Compton scattering in the framework of baryon
chiral perturbation theory (BχPT) with pion, nucleon, and Δ(1232)
degrees of freedom, up to and including the next-to-next-to-leading order
(NNLO). We include the effects of order p2, p3 and p4/Δ, with
Δ≈300 MeV the Δ-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, p4). Estimating the theoretical
uncertainty on the basis of natural size for p4 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)×10−4 fm3, in
significant disagreement with the current PDG value. Unlike the previous
χPT 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 HBχPT and BχPT
results for polarizabilities is found to be appreciable. We discuss the chiral
behavior of proton polarizabilities in both HBχPT and BχPT 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