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Ironically, although 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 greater. FLOATSUBSCRIPTCl. At zero subject, six distinct magnetic sublattices may be recognized, which would presumably result in six distinct magnon branches; nonetheless, as a result of canted nature of the copper ions occupying the 4(c) websites, the exact number of branches might differ from six. Brillouin zone center crossing of two magnon dispersion curves along orthogonal directions, however inelastic neutron scattering measurements are wanted to research further the excitation’s seemingly isotropic existence. FLOATSUPERSCRIPT at 5 Ok. Now we have tentatively assigned the magnetic excitation to a magnon based on analysis of beforehand reported oscillator strengths of magnons and electromagnons. FLOATSUPERSCRIPT excitation (at 1 T) splits beneath the metamagnetic transition; however, under 1 T experimental limitations prevented us from tracking the excitation. Generalizing this theory, which was labored out for two sublattices, to a scenario with greater than two sublattices, we will 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 concept.

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