interaction in leading order covariant chiral effective field theory
arXiv:2010.06916 · doi:10.1103/PhysRevC.102.065208
Abstract
We study the interaction in the covariant chiral effective field theory (ChEFT) at leading order. All the relevant low-energy constants are determined by fitting to the lattice QCD simulations from the HAL QCD Collaboration. Extrapolating the results to the physical point, we show that the interaction is weakly attractive in the channel, but in the channel, it is only attractive at extremely low energies and soon turns repulsive for larger laboratory energy. Furthermore, we show that the neglect of the coupling provided by the leading order covariant ChEFT would result in an attractive interaction in the channel at the physical point, which coincides with the previous non-relatistic ChEFT study. As a byproduct, we predict the phase shifts and the mixing angel , which can be checked by future lattice QCD simulations. In addition, we compare the interaction with the and interactions to study how the baryon-nucleon () interactions evolve as a function of the baryon mass with the replacement of a light quark by a strange or charm quark in the baryon ().
10 pages, 7 figures
References in corpus (5)
Cited by in corpus (5)
- Chiral perturbation theory for heavy hadrons and chiral effective field theory for heavy hadronic molecules
- Precision Studies of QCD in the Low Energy Domain of the EIC
- Accurate relativistic chiral nucleon-nucleon interaction up to NNLO
- Strangeness baryon-baryon interactions and femtoscopic correlation functions in covariant chiral effective field theory
- Nonperturbative two-pion exchange contributions to the nucleon-nucleon interaction in covariant baryon chiral perturbation theory