TY - JOUR
T1 - Microscopic calculations based on chiral two- and three-nucleon forces for proton- and He 4 -nucleus scattering
AU - Toyokawa, Masakazu
AU - Yahiro, Masanobu
AU - Matsumoto, Takuma
AU - Minomo, Kosho
AU - Ogata, Kazuyuki
AU - Kohno, Michio
N1 - Publisher Copyright:
© 2015 American Physical Society. ©2015 American Physical Society.
PY - 2015/8/25
Y1 - 2015/8/25
N2 - We investigate the effects of chiral three-nucleon force (3NF) on proton scattering at 65 MeV and He4 scattering at 72 MeV/nucleon from heavier targets, using the standard microscopic framework composed of the Brueckner-Hartree-Fock (BHF) method and the g-matrix folding model. For nuclear matter, the g matrix is evaluated from chiral two-nucleon force (2NF) of N3LO and chiral 3NF of NNLO by using the BHF method. Because the g matrix thus obtained is numerical and nonlocal, an optimum local form is determined from the on-shell and near-on-shell components of g matrix that are important for elastic scattering. For elastic scattering, the optical potentials are calculated by folding the local chiral g matrix with projectile and target densities. This microscopic framework reproduces the experimental data without introducing any adjustable parameter. Chiral-3NF effects are small for proton scattering, but sizable for He4 scattering at middle angles where the data are available. Chiral 3NF, mainly in the 2π-exchange diagram, makes the folding potential less attractive and more absorptive for all the scattering.
AB - We investigate the effects of chiral three-nucleon force (3NF) on proton scattering at 65 MeV and He4 scattering at 72 MeV/nucleon from heavier targets, using the standard microscopic framework composed of the Brueckner-Hartree-Fock (BHF) method and the g-matrix folding model. For nuclear matter, the g matrix is evaluated from chiral two-nucleon force (2NF) of N3LO and chiral 3NF of NNLO by using the BHF method. Because the g matrix thus obtained is numerical and nonlocal, an optimum local form is determined from the on-shell and near-on-shell components of g matrix that are important for elastic scattering. For elastic scattering, the optical potentials are calculated by folding the local chiral g matrix with projectile and target densities. This microscopic framework reproduces the experimental data without introducing any adjustable parameter. Chiral-3NF effects are small for proton scattering, but sizable for He4 scattering at middle angles where the data are available. Chiral 3NF, mainly in the 2π-exchange diagram, makes the folding potential less attractive and more absorptive for all the scattering.
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U2 - 10.1103/PhysRevC.92.024618
DO - 10.1103/PhysRevC.92.024618
M3 - Article
AN - SCOPUS:84940866085
SN - 0556-2813
VL - 92
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 2
M1 - 024618
ER -