Abstract
One of the two key requirements of
n-dimensional ferroic systems is the spontaneous formation of homogeneously ordered areas, called domains, separated one from another by distinct (
\(n-1\))-dimensional entities, called domain walls, see Sect.
2.1.4 on page
16. These walls constitute natural interfaces within the system between two or more energetically degenerate realisations of a particular order. For the artificial nanomagnetic arrays investigated throughout this work, the spontaneous formation of long-range order connected to an order parameter is a hallmark for their classification as primary ferroic order [
1]. Suitable symmetry groups allowing for toroidal order have already been identified a few decades ago and are listed in Sect.
2.1.6 on page
19. The nanomagnetic arrays that have been investigated here, see Fig.
4.1 on page
83, fall in one of these groups, setting the basis for their further scrutiny not only on the macroscopic but also on the microscopic scale.