Abstract
We calculate the energy spectrum of a bound S1⁄2 proton in the JPT = I+0 ground state of Li 6. We use the K harmonics formulation in Kmin approximation. A continuous negative energy spectrum is obtained. This is in contrast to the simple shell model where a discrete delta function negative energy distribution is an input assumption of the model. The energy speCtrum of a bound nucleon is similar, yet complementary, to the energy spectral function of an excited hole state of a nucleus. Because of our interest in (0s1⁄2) proton pickup or knockout reactions in light nuclei we choose to focus our attention on the energy distribution of a proton in a target nucleus, rather than for a hole in a highly excited residual nucleus. We write the hamiltonian for the entire system as
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