Abstract
The magnetic dipole strength and energy-weighted strength distribution is calculated in 8Be, as well as the separate orbit and spin parts. All ΔN = 2 excitations over and above (and including) the configuration 0s 40p 4 are included. The interaction has a central, two-body spin-orbit and a tensor part. The energy-independent and energy-weighted orbital strength distribution is remarkably insensitive to the presence or ansence of the spin-orbit or tensor interaction — not so the spin strength. The energy-weighted strength distribution can be divided into a low energy and a high energy part. The high energy orbital part is somewhat less but close to the low energy part. There is a wide plateau separating the low energy part from the high energy part.
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