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Cause of deterioration of N^3LO predictions at ~100 MeV in Long–Yang MWPC

Determine whether the decline in order-by-order improvement observed near a laboratory scattering energy of approximately 100 MeV for neutron–proton scattering observables computed up to next-to-next-to-next-to-leading order in the modified Weinberg power counting of Long and Yang—where sub-leading potential corrections are included perturbatively—is caused by overfitting of the calibrated low-energy constants or by an inherent deficiency in the modified Weinberg power counting itself.

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Background

The paper computes neutron–proton scattering observables up to N3LO using a renormalization-group invariant modified Weinberg power counting (MWPC) by Long and Yang, in which one-pion exchange is treated non-perturbatively in specific channels and higher-order corrections enter via distorted-wave perturbation theory. Low-energy constants (LECs) are calibrated to selected Nijmegen phase shifts, and calculations are performed for two cutoffs (500 and 2500 MeV).

The authors report steady order-by-order convergence and realistic descriptions up to roughly 60 MeV. However, around 100 MeV, some N3LO predictions do not improve over N2LO for differential cross sections and certain polarizations. They explicitly state uncertainty about the origin of this deterioration, raising two possibilities: overfitting of LECs or an underlying issue with the adopted MWPC. Identifying the cause is important for assessing the robustness and predictive power of RG-invariant chiral EFT in this energy regime.

References

Indeed, for T_lab≈100 MeV (rightmost panels of \cref{fig:np_obs_ang}), it appears that the order-by-order improvement in the predictions of the differential cross section and P_b polarization deteriorates and \NNLO{} can perform better than \NNNLO. It is not clear at the moment if this is due to overfitting and (or) an underlying issue with the MWPC that we employ.

Perturbative computations of neutron-proton scattering observables using renormalization-group invariant $χ$EFT up to N$^3$LO (2402.15325 - Thim et al., 23 Feb 2024) in Section 3 (Neutron-Proton Scattering Observables)