On the Nuclear Two-, Three- and Four-Body Problems

Abstract
The simplest nuclear Hamiltonian satisfying all present requirements includes a Majorana-Heisenberg interaction {(1g)P+gPQ}V(r) between unlike particles and an attractive singlet interaction between like particles which is equal to that for unlike particles. The experimental mass defects of H2 and H3 together with the cross section σ for slow neutron-proton scattering will determine the range b and depth B of the triplet well and the proportion g of Heisenberg force (we use throughout the potential Be2rb). An exact analytic expression relating σ, b, B and g is derived for this potential and g is found to be very insensitive to σ. An exact solution of H2 gives the relation between B and b. The final relation which fixes the parameters is furnished by a Ritz-Hylleraas variational treatment of H3 with the above Hamiltonian and the wave function: ψ=212α1(α2β3α3β2)φ1+612(α1(α2β3+α3β2)2β1α2α3)φ2 where φ1 and φ2 each represents an exponential times a power series in the interparticle distances of proper symmetry φ2 is brought in by the Heisenberg term; the Breit-Feenberg operator is used for the small triplet like-particle interaction). The convergence of energies obtained from successive improvements in ψ is rapid and the eigenvalue may be closely estimated. After a relativistic correction is made we obtain: b=1.73×1013 cm; B=242 mc2 and

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