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Prog. Theor. Phys. Supplement No.56 (1974) pp. 6-31

[ Full Text PDF : FREE ACCESS (1479K) ]

Chapter II. The ATMS Method and the Three-Nucleon System with Realistic Potentials

Yoshinori Akaishi, Motoki Sakai, Jun Hiura* and Hajime Tanaka

Department of Physics, Hokkaido University, Sapporo
*College of Liberal Arts, Iwate University, Morioka

(Received February 3, 1975)

Abstract:

The ATMS method, which is a variational one, is explained. The wave function is constructed from the two-body scattering correlations on the basis of the multiple scattering theory. The triton is treated with the Hamada-Johnston (H-J), the Tamagaki (OPEH and OPEG) and Wada and Obinata's (OBEV) potentials. The upper-bound energies are -6.00 MeV for H-J, -6.59 MeV for OPEH, -6.64 MeV for OPEG and -5.91 MeV for OBEV. The kinetic energies are 66 MeV for H-J and 33 MeV for OBEV. The tensor force in the triplet-even state has the largest contribution which amounts to -38 MeV for H-J. The Coulomb energy of 3He is estimated. The two-body wave function is drawn out from the wave function of the triton. The ATMS method is powerful in solving the three-nucleon problem with realistic potentials.


URL : http://ptp.ipap.jp/link?PTPS/56/6/
DOI : 10.1143/PTPS.56.6

[ Full Text PDF : FREE ACCESS (1479K) ] Citation:

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