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Ironically, though the metamagnetic transition successfully reduces the variety of magnetic sublattices from six to a few, we observe an extra magnetic excitation appearing at fields of 1 T and larger. FLOATSUBSCRIPTCl. At zero field, six distinct magnetic sublattices can be recognized, which might presumably lead to six distinct magnon branches; nonetheless, as a result of canted nature of the copper ions occupying the 4(c) sites, the precise number of branches could differ from six. Brillouin zone heart crossing of two magnon dispersion curves alongside orthogonal directions, however inelastic neutron scattering measurements are wanted to investigate additional the excitation’s seemingly isotropic existence. FLOATSUPERSCRIPT at 5 Ok. We now have tentatively assigned the magnetic excitation to a magnon primarily based on analysis of previously 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 monitoring the excitation. Generalizing this idea, which was worked out for two sublattices, to a scenario with greater than two sublattices, we can see that the dispersion of the excitation we observe (inset of Fig. 5b) is in qualitative agreement (i.e., both are non-linear) with the lower frequency department predicted by the AFMR idea.

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