either excite two particles to the next major shell or excite one particle through two major shells. We also give results for the summed strength in the [*low-large space*]{} -this is the low energy part of the large space covering an energy range more or less equal to that of the small space. It is easy to identify the low energy sector because there is a fairly wide plateau in the summed strength which separates the low energy rise from the high energy rise.

Usually the large space summed strength is somewhat larger than the small space strength e.g. for the isovector orbital strength in $^8\mbox{Be}$ the values shown in Table $I$ are $0.6701$ $\mu_N^2$ and $0.7283$ $\mu_N^2$ respectively. But there is one glaring exception. For the case of $J^{\pi}=0^+$ $T=1$ $\rightarrow$ $J^{\pi}=1^+$ $T=1$ transitions in $^{10}\mbox{Be}$, the summed isovector spin strength in the large space is $2.08~10^{-2}$ $\mu_N^2$ but in the small space it is $2.34~10^{-2}$ $\mu_N^2$. For the orbital strength it is the other way around but for the physical case ($g_{l\pi}=1$, $g_{l\nu}=0$, $g_{s\pi}=5.586$, $g_{s\nu}=-3.826$) the spin prevails and the summed strength in the $1.952$ $\mu_N^2$ is less than in the $2.09$ $\mu_N^2$.

Thus it is not always 