“…We start with the realization that to minimize the very large exchange energy (>0.4 eV) [23,24] associated with domain walls, it is clearly advantageous for the nodal planes (where the spin polarization vanishes) of the SDW with its propagation vector perpendicular to the domain wall to lie on the walls [25]. Such an assumption is further supported by the previously observed preference for the formation of SDW nodes at Fe/Cr interfaces [26].…”
“…We start with the realization that to minimize the very large exchange energy (>0.4 eV) [23,24] associated with domain walls, it is clearly advantageous for the nodal planes (where the spin polarization vanishes) of the SDW with its propagation vector perpendicular to the domain wall to lie on the walls [25]. Such an assumption is further supported by the previously observed preference for the formation of SDW nodes at Fe/Cr interfaces [26].…”
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