Consequences of omitting spin-orbit partner configurations for $B\left(E2\right)$ values and quadrupole moments in nuclei

Shell-model calculations of $B\left(E2\right)$'s and quadrupole moments in the even-even nuclei in the $g_{9/2}$ shell region below ${}^{100}\mathrm{Sn}$ are hampered by the fact that the inclusion of the $g_{7/2}$ configuration will lead to model spaces that are too large to handle. Understanding the impact of specific orbit wave functions in large-scale shell-model (LSSM) calculations helps to shed light on the validity of the results that are obtained. We therefore examine lighter nuclei in the beginning of the $fp$ region where one can normally include all the orbitals, $f_{7/2},p_{3/2},p_{1/2}$, and $f_{5/2}$, for both protons and neutrons. We perform such calculations but then take a step back and exclude the $f_{5/2}$ orbital. By comparing the results of the two calculations we can hope to get insight into the importance of the missing spin-orbital partner in other regions.