We update the predictions of the SU(2) baryon chiral perturbation theory for
the dipole polarisabilities of the proton,
{αE1,βM1}p={11.2(0.7),3.9(0.7)}×10−4fm3,
and obtain the corresponding predictions for the quadrupole, dispersive, and
spin polarisabilities:
{αE2,βM2}p={17.3(3.9),−15.5(3.5)}×10−4fm5,
{αE1ν,βM1ν}p={−1.3(1.0),7.1(2.5)}×10−4fm5,
and
{γE1E1,γM1M1,γE1M2,γM1E2}p={−3.3(0.8),2.9(1.5),0.2(0.2),1.1(0.3)}×10−4fm4.
The results for the scalar polarisabilities are in significant disagreement
with semi-empirical analyses based on dispersion relations, however the results
for the spin polarisabilities agree remarkably well. Results for proton
Compton-scattering multipoles and polarised observables up to the Delta(1232)
resonance region are presented too. The asymmetries Σ3 and
Σ2x reproduce the experimental data from LEGS and MAMI. Results for
Σ2z agree with a recent sum rule evaluation in the forward
kinematics. The asymmetry Σ1z near the pion production threshold
shows a large sensitivity to chiral dynamics, but no data is available for this
observable. We also provide the predictions for the polarisabilities of the
neutron:
{αE1,βM1}n={13.7(3.1),4.6(2.7)}×10−4fm3,
{αE2,βM2}n={16.2(3.7),−15.8(3.6)}×10−4fm5,
{αE1ν,βM1ν}n={0.1(1.0),7.2(2.5)}×10−4fm5,
and
{γE1E1,γM1M1,γE1M2,γM1E2}n={−4.7(1.1),2.9(1.5),0.2(0.2),1.6(0.4)}×10−4fm4.
The neutron dynamical polarisabilities and multipoles are examined too. We also
discuss subtleties related to matching dynamical and static polarisabilities.Comment: 34 pages, 18 figures, minor updates and corrections, published
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