Project Chaos

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Ironically, though the metamagnetic transition successfully reduces the variety of magnetic sublattices from six to 3, we observe an extra magnetic excitation showing at fields of 1 T and greater. FLOATSUBSCRIPTCl. At zero subject, six distinct magnetic sublattices can be recognized, which might presumably result in six distinct magnon branches; however, because of the canted nature of the copper ions occupying the 4(c) websites, the precise number of branches could differ from six. Brillouin zone middle crossing of two magnon dispersion curves alongside orthogonal instructions, but inelastic neutron scattering measurements are wanted to analyze further the excitation’s seemingly isotropic existence. FLOATSUPERSCRIPT at 5 K. We have now tentatively assigned the magnetic excitation to a magnon based on evaluation of beforehand reported oscillator strengths of magnons and electromagnons. FLOATSUPERSCRIPT excitation (at 1 T) splits beneath the metamagnetic transition; nevertheless, under 1 T experimental limitations prevented us from monitoring the excitation. Generalizing this concept, which was worked out for two sublattices, to a state of affairs with more than two sublattices, we are able to see that the dispersion of the excitation we observe (inset of Fig. 5b) is in qualitative settlement (i.e., each are non-linear) with the lower frequency branch predicted by the AFMR concept.

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