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Figure 2
Magnetic structures giving rise to the magnetoelectric effect resulting from the action of the OP(a,b,c[\mid]d,e,f) transforming as mX3+ [\oplus] mX1-, shown along the high-symmetry directions OP(a,0,0[\mid]d,0,0), OP(a,a,0[\mid]d,d,0), OP(a,[\bar{a}],a[\mid]d,[\bar{d}],d).

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