For the plot concerning the low-spin iron, the splitting of the states is much clearer compared to the high-spin iron. This is one cluster of states around -2 eV that represent the a 1g /e g -states of low-spin iron and a second cluster of states starting at +2 eV that can be ascribed to the e g -states. Due to these states being either completely filled or empty, no shift between the majority and minority spin states can be observed. vious paragraph, the calculations for both, cubic and rhombohedral Prussian white, are in accordance with the experiment on PW being a conductor. We also address the magnetization of both iron species for cubic and rhombohedral PW. Both phases are showing a clear distinction between the irons, matching the experimentally seen high-spin-low-spin configuration. Furthermore, the total amount of magnetization matches the formally expected values within the expected error margins.