Strangeness and baryon-baryon interactions in relativistic chiral effective field theory
arXiv:2011.05510 · doi:10.1103/PhysRevC.103.025201
Abstract
The strangeness and baryon-baryon interactions are investigated in the relativistic chiral effective field theory at leading order. First, the potentials are derived from the sector assuming that the corresponding low-energy constants are related to each other via SU(3) flavor symmetry. The comparison with the state-of-the-art lattice QCD simulations, show, however, that SU(3) flavor symmetry breaking effects can not be neglected. In order to take into account these effects, we redetermine two sets of low-energy constants by fitting to the lattice QCD data in the and channels respectively. The fitting results demonstrate that the lattice QCD -waves phase shifts for both channels can be described rather well. Without any additional free low-energy constants, the predicted phase shifts for the channel and the mixing angle are also in qualitative agreement with the lattice QCD data for the channel, while the results for the channel remain to be checked by future lattice QCD simulations. With the so-obtained low-energy constants, the -wave scattering lengths and effective ranges are calculated for these two channels at the physical point. Finally, in combination with the and results obtained in our previous works, we study the evolution of the irreducible representation in the baryon-baryon interactions as a function of increasing strangeness. It is shown that the attraction decreases dramatically as strangeness increases from to , but then remains relatively stable until . The results indicate that the existence of bound states in the and channels is rather unlikely.
9 pages, 4 figures
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Cited by in corpus (5)
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- Quenched Λ spin-orbit splitting by relativistic Fock diagram in single-Λ hypernuclei
- Impact of -Hypernuclear Constraints on Relativistic Equation of State and Properties of Hyperon Stars