Abstract

Conical refraction, which is due to the renormalization of the elastic moduli by the effective magnetoelastic interaction and depends on the static magnetic field, has been experimentally observed in an α-Fe2O3 trigonal easy-plane antiferromagnet in addition to the usual internal conical refraction of transverse elastic waves propagating along the trigonal C3 axis. It has been shown that the deviation angle θη of the energy flux from the C3 axis at the internal conical refraction is independent of the magnetic field applied in the basal plane (H ⊥ C3) and is a constant determined by the ratio of the elastic moduli C14 and C44. The deviation angle of the energy flux at the antiferromagnetic conical refraction increases with the magnetic field and approaches the value θη at large H values. The results are well described by the theory of this phenomenon developed by E.A. Turov and confirm its basic conclusions.

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