A big advantage of sDFT in practical calculations is that charge and spin state of every subsystem can be specified by the user. This can be used, for instance, to converge aggregates of open-shell subsystems to arbitrary local-spin patterns in an almost trivial manner . In KS-DFT calculations, this often causes problems either due to the overdelocalization error or simply due to problems to converge to a desired spin distribu-tion.