Speaker
Description
We have been performing calculations [1] using the SMS chiral potential [2] for NN interactions, the Juelich NLO19 chiral potential [3] for YN interactions, and the YNN three-body force [4] as inputs for the Faddeev three-body equations of Hypertriton. For the YNN three-body force, not only a two-pion exchange type but also one-pion exchange and contact types were adopted. Partial wave expansion [5] was performed to examine [6] the effects of each type. It is known that in chiral NLO order, it is not possible to determine the low-energy coefficients (LECs) of the three-body force, but the range dependence of the high momentum cutoff is examined.
[1] H. Kamada, M. Kohno and K. Miyagawa, Phys. Rev. C 108, no.2, 024004 (2023)
[2] P. Reinert, H. Krebs and E. Epelbaum, Eur. Phys. J. A 54, no.5, 86 (2018)
[3] J. Haidenbauer, U.-G. Meißner and A. Nogga, Eur. Phys. J. A 56, no.3, 91 (2020)
[4] S. Petschauer, N. Kaiser, J. Haidenbauer, U.-G. Meißner and W. Weise, Phys. Rev. C 93, no.1, 014001 (2016)
[5] M. Kohno, H. Kamada and K. Miyagawa, Phys. Rev. C 106, no.5, 054004 (2022)
[6] M. Kohno, H. Kamada and K. Miyagawa, Phys. Rev. C 109, no.2, 024003 (2024)
