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Ironically, though the metamagnetic transition effectively reduces the number of magnetic sublattices from six to three, we observe a further magnetic excitation appearing at fields of 1 T and larger. FLOATSUBSCRIPTCl. At zero subject, six distinct magnetic sublattices will be identified, which would presumably result in six distinct magnon branches; nevertheless, as a result of canted nature of the copper ions occupying the 4(c) websites, the exact number of branches may differ from six. Brillouin zone center crossing of two magnon dispersion curves alongside orthogonal directions, however inelastic neutron scattering measurements are wanted to research additional the excitation’s seemingly isotropic existence. FLOATSUPERSCRIPT at 5 K. We now have tentatively assigned the magnetic excitation to a magnon based on evaluation of previously reported oscillator strengths of magnons and electromagnons. FLOATSUPERSCRIPT excitation (at 1 T) splits beneath the metamagnetic transition; nonetheless, below 1 T experimental limitations prevented us from tracking the excitation. Generalizing this principle, which was worked out for two sublattices, to a scenario with more than two sublattices, we can see that the dispersion of the excitation we observe (inset of Fig. 5b) is in qualitative settlement (i.e., both are non-linear) with the lower frequency department predicted by the AFMR theory.

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