Second-order perturbation theory for 3He and pd scattering in pionless EFT
arXiv:1609.03163 · doi:10.1088/1361-6471/aa60d6
Abstract
This work implements pionless effective field theory with the two-nucleon system expanded around the unitarity limit at second order perturbation theory. The expansion is found to converge well. All Coulomb effects are treated in perturbation theory, including two-photon contributions at next-to-next-to-leading order. After fixing a three-nucleon force to the 3He binding energy at this order, proton-deuteron scattering in the doublet S-wave channel is calculated for moderate center-of-mass momenta.
24 pages, 7 figures, published version
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Cited by in corpus (14)
- Nuclear effective field theory: status and perspectives
- Nuclear Physics Around the Unitarity Limit
- Naturalness in Nuclear Effective Field Theories
- Charge and Magnetic Properties of Three-Nucleon Systems in Pionless Effective Field Theory
- Energies and radii of light nuclei around unitarity
- Clustering of Four-Component Unitary Fermions
- A Consistency Test of EFT Power Countings from Residual Cutoff Dependence
- Five-body calculation of -wave -He scattering at next-to-leading order pionless effective field theory
- What Can Possibly Go Wrong?
- Few nucleons scattering in pionless effective field theory
- A Vision for the Science of Rare Isotopes
- Renormalization of proton-proton fusion in chiral effective field theory
- Cold Neutron-Deuteron Capture and Wigner-SU(4) Symmetry
- Two-Body Triton Photodisintegration and Wigner-SU(4) Symmetry