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Ironically, although the metamagnetic transition successfully reduces the variety of magnetic sublattices from six to 3, we observe an additional magnetic excitation appearing at fields of 1 T and higher. FLOATSUBSCRIPTCl. At zero field, six distinct magnetic sublattices will be recognized, which might presumably lead to six distinct magnon branches; however, due to the canted nature of the copper ions occupying the 4(c) sites, the precise number of branches might differ from six. Brillouin zone center crossing of two magnon dispersion curves along orthogonal instructions, however inelastic neutron scattering measurements are needed to investigate further the excitation’s seemingly isotropic existence. FLOATSUPERSCRIPT at 5 K. We have now tentatively assigned the magnetic excitation to a magnon based mostly on analysis of beforehand reported oscillator strengths of magnons and electromagnons. FLOATSUPERSCRIPT excitation (at 1 T) splits beneath the metamagnetic transition; nevertheless, below 1 T experimental limitations prevented us from tracking the excitation. Generalizing this concept, which was labored out for 2 sublattices, to a situation with more than two sublattices, we can see that the dispersion of the excitation we observe (inset of Fig. 5b) is in qualitative agreement (i.e., each are non-linear) with the decrease frequency department predicted by the AFMR idea.

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