Nuclear forces can be systematically derived using effective chiral Lagrangians consistent with the symmetries of QCD. I review the status of the calculations for two- and three-nucleon forces and their applications in few-nucleon systems. I also address issues like the quark mass dependence of the nuclear forces and resonance saturation for four-nucleon operators.

/pdf/modern-theory-of-nuclear-forces-436h635pm0.pdf

Modern theory of nuclear forces

Special Functions and Their Applications. By N. N. Lebedev, translated by R. A. Silverman. Pp. xii, 308. 96s. 1965. (Prentice-Hall)

Energy levels of light nuclei A=8,9,10

https://www.cns.s.u-tokyo.ac.jp/~shimoura/research/nuc_data/pdf/11.pdf

Energy levels of light nuclei A = 11-12

Gaussian expansion method for few-body systems

Chapter II. Comprehensive Study of Alpha-Nuclei

Baryon–baryon interactions in the SU6 quark model and their applications to light nuclear systems

Interactions between the octet-baryons (B8) in the spin-flavor SU6 quark model are investigated in a unified coupled-channels framework of the resonating-group method (RGM). The interaction Hamiltonian for quarks consists of the phenomenological confinement potential, the color Fermi-Breit interaction with explicit flavor-symmetry breaking (FSB), and effective-meson exchange potentials of scalar-, pseudoscalar- and vector-meson types. The model parameters are determined to reproduce the properties of the nucleon-nucleon (NN) system and the low-energy cross section data for the hyperon-nucleon (YN) interactions. The NN phase shifts and many observables for the NN and YN interactions are nicely reproduced. Properties of these B8 B8 interactions are analyzed through the G-matrix calculations. The B8 B8 interactions are then applied to some of few-baryon systems and light Lambda-hypernuclei in a three-cluster Faddeev formalism using two-cluster RGM kernels. An application to the three-nucleon system shows that the quark-model NN interaction can give a sufficient triton binding energy with little room for the three-nucleon force. The hypertriton Faddeev calculation indicates that the attraction of the Lambda N interaction in the 1S0 state is only slightly more attractive than that in the 3S1 state. In the application to the alpha alpha Lambda system, the energy spectrum of 9 Lambda Be is well reproduced using the alpha alpha RGM kernel. The very small spin-orbit splitting of the 9 Lambda Be excited states is also discussed. In the Lambda Lambda alpha Faddeev calculation, the NAGARA event for 6 Lambda Lambda He is found to be consistent with the quark-model Lambda Lambda interaction.

Baryon-baryon interactions in the SU6 quark model and their applications to light nuclear systems

A simultaneous description of the {ital NN} and {ital YN} interactions is attempted in the resonating-group formulation of the spin-flavor SU{sub 6} quark model, in which the full Fermi-Breit interaction with explicit quark-mass dependence acts between quarks, and all the mesons of scalar and pseudo-scalar nonets couple directly to quarks. An overall agreement with the existing data is obtained with few adjustable parameters. In the {Lambda}{ital p} elastic total cross sections, the cusp structure at the {Sigma}{ital N} threshold is strongly enhanced by the antisymmetric {ital LS}{sup ({minus})} force generated from the Fermi-Breit interaction. {copyright} {ital 1996 The American Physical Society.}

Unified description of NN and YN interactions in a quark model with effective meson-exchange potentials.

Baryon-baryon interactions for the complete baryon octet ${(B}_{8})$ are investigated in a unified framework of the resonating-group method, in which the spin-flavor ${\mathrm{SU}}_{6}$ quark-model wave functions are employed Model parameters are determined to reproduce properties of the nucleon-nucleon system and the low-energy cross section data for the hyperon-nucleon interaction We then proceed to explore ${B}_{8}{B}_{8}$ interactions in the strangeness $S=\ensuremath{-}2,$ $\ensuremath{-}3,$ and $\ensuremath{-}4$ sectors The S-wave phase-shift behavior and total cross sections are systematically understood by (1) the spin-flavor ${\mathrm{SU}}_{6}$ symmetry, (2) the special role of the pion exchange, and (3) the flavor symmetry breaking

/pdf/interactions-between-octet-baryons-in-the-su-6-quark-model-1zydnvcva5.pdf

Yoshikazu Fujiwara

Papers

Chapter II. Comprehensive Study of Alpha-Nuclei

Baryon–baryon interactions in the SU6 quark model and their applications to light nuclear systems

Baryon-baryon interactions in the SU6 quark model and their applications to light nuclear systems

Unified description of NN and YN interactions in a quark model with effective meson-exchange potentials.

Interactions between octet baryons in the SU 6 quark model