Perturbational and variational calculations with single-particle Legendre functions have been made for the nuclear five-body problem of He⁵. The symmetric Hamiltonian is employed; the values of the nuclear parameters chosen favor high binding. With a symmetric interaction, Li⁵ and He⁵ differ only in the Coulomb energy, states of the former lying about one Mev above those of the latter. The calculations show that there is no state of He⁵ which is stable against dissociation into an alpha-particle and a neutron. There are two low-lying virtual levels, one of ²P, the other of ²S symmetry; according to the Hartree model, the energies of these states are -11.7 and -6.5 Mev, respectively. Second-order perturbation calculations diminish the interval ²S-²P radically and locate both the states in the neighborhood of -19.0 Mev. The last two results are roughly confirmed by variational calculations with two variation parameters (alpha-particle model), and -20 Mev may be set as a probable lower bound to the position of either state. These estimated values fall some seven Mev short of the experimental energy.
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Warren A. Tyrrell (1939) studied this question.
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