Trinucleon bound-state properties from an exact solution of the Faddeev equations with realistic nuclear forces
EP Harper, YE Kim, A Tubis - Physical Review Letters, 1972 - APS
EP Harper, YE Kim, A Tubis
Physical Review Letters, 1972•APSThe trinucleon bound-state energy, wave function, and charge form factor are calculated
from a direct solution of the complete set of Faddeev equations. The nucleon-nucleon
interaction (effective in the S 0 1 and S 1 3− D 1 3 states) is given by the Reid soft-core
potential. We find EB= 6.7 MeV, P (S)= 89.7%, P (S′)= 1.7%, and P (D)= 8.6%.| F Ch He 3
(Q 2)|(calculated) is similar to the approximate result of Tjon, Gibson, and O'Connell, and
has a minimum at Q 2= 15.5 fm− 2.
from a direct solution of the complete set of Faddeev equations. The nucleon-nucleon
interaction (effective in the S 0 1 and S 1 3− D 1 3 states) is given by the Reid soft-core
potential. We find EB= 6.7 MeV, P (S)= 89.7%, P (S′)= 1.7%, and P (D)= 8.6%.| F Ch He 3
(Q 2)|(calculated) is similar to the approximate result of Tjon, Gibson, and O'Connell, and
has a minimum at Q 2= 15.5 fm− 2.
Abstract
The trinucleon bound-state energy, wave function, and charge form factor are calculated from a direct solution of the complete set of Faddeev equations. The nucleon-nucleon interaction (effective in the S 0 1 and S 1 3− D 1 3 states) is given by the Reid soft-core potential. We find E B= 6.7 MeV, P (S)= 89.7%, P (S′)= 1.7%, and P (D)= 8.6%.| F Ch He 3 (Q 2)|(calculated) is similar to the approximate result of Tjon, Gibson, and O'Connell, and has a minimum at Q 2= 15.5 fm− 2.
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