TY - JOUR
T1 - Towards modeling cluster structure of 8Be with chiral interaction
AU - Fukui, Tokuro
N1 - Funding Information:
The author thanks N Itagaki for helpful advice and providing a numerical code of the Brink model. He also thanks M Kamimura for supplying a numerical code to calculate the scattering phase shift, and R Machleidt for parameterizing the LECs. He is grateful to Y Yamaguchi for fruitful discussions. This work was supported in part by JSPS KAKENHI Grant No. JP21K13919. The calculations have been carried out using the computer facilities at Yukawa Institute for Theoretical Physics, Kyoto University, and Research Center for Nuclear Physics, Osaka University.
Publisher Copyright:
© 2022 The Author(s). Published by IOP Publishing Ltd.
PY - 2022/5
Y1 - 2022/5
N2 - How the nuclear force behaves in cluster states, in particular those consisting of the α clusters, has been investigated so far, but not yet elucidated. Today the chiral effective field theory (EFT) is established and it would shed new light on the microscopic understanding of the cluster states. We aim to address a possible source of the attraction in the cluster states of 8Be in view of the pion exchange. Namely, we investigate whether the two-pion-exchange interaction acts as a dominant attraction in the α + α system as predicted by a previous work. We describe theoretically the cluster structure of 8Be by the Brink model, for which the effective interaction is designed from the realistic nuclear force derived through the chiral EFT. The two-body matrix elements of the chiral interaction with the local-Gaussian bases are formulated within the approximation of the spin-isospin saturation forming an α particle. Introducing a global prefactor to the chiral interaction phenomenologically, the ground and low-lying excited states of 8Be, the scattering phase shift of the α-α system as well, are satisfactorily depicted. The attraction in the cluster states is found to be stemming from the two-pion-exchange contributions dominantly, along with nonnegligible short-range terms. The present work can be the foundation towards constructing realistic cluster models, by which the cluster states will be revealed microscopically in the next step.
AB - How the nuclear force behaves in cluster states, in particular those consisting of the α clusters, has been investigated so far, but not yet elucidated. Today the chiral effective field theory (EFT) is established and it would shed new light on the microscopic understanding of the cluster states. We aim to address a possible source of the attraction in the cluster states of 8Be in view of the pion exchange. Namely, we investigate whether the two-pion-exchange interaction acts as a dominant attraction in the α + α system as predicted by a previous work. We describe theoretically the cluster structure of 8Be by the Brink model, for which the effective interaction is designed from the realistic nuclear force derived through the chiral EFT. The two-body matrix elements of the chiral interaction with the local-Gaussian bases are formulated within the approximation of the spin-isospin saturation forming an α particle. Introducing a global prefactor to the chiral interaction phenomenologically, the ground and low-lying excited states of 8Be, the scattering phase shift of the α-α system as well, are satisfactorily depicted. The attraction in the cluster states is found to be stemming from the two-pion-exchange contributions dominantly, along with nonnegligible short-range terms. The present work can be the foundation towards constructing realistic cluster models, by which the cluster states will be revealed microscopically in the next step.
UR - http://www.scopus.com/inward/record.url?scp=85130109752&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85130109752&partnerID=8YFLogxK
U2 - 10.1088/1361-6471/ac58b3
DO - 10.1088/1361-6471/ac58b3
M3 - Article
AN - SCOPUS:85130109752
SN - 0954-3899
VL - 49
JO - Journal of Physics G: Nuclear and Particle Physics
JF - Journal of Physics G: Nuclear and Particle Physics
IS - 5
M1 - 055102
ER -