Abstract
The weak ferromagnet FeBO3 exhibits a strong dependence of the transverse sound velocity on the external magnetic field. This dependence has been measured for phonons up to the GHz region. The results can be explained satisfactorily by the interaction of the phonon and magnon dispersion branches.
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References
See, e.g., R. C. LeCraw, R. L. Comstock: InPhysical Acoustics Vol. IIIB, ed. by W. P. Mason (Academic Press, New York 1965) pp. 127–199
P. P. Maksimenkov, V. J. Ozhogin: Sov. Phys. JETP38, 324–328 (1974)
W. Jantz, W. Wettling: Appl. Phys.15, 399–407 (1978)
W. Jantz, J. R. Sandercock, W. Wettling: J. Phys. C (Solid State Phys.)9, 2229–2240 (1976)
R. Wolfe, A. J. Kurtzig, R. C. LeCraw: J Appl. Phys.41, 1218–1224 (1970)
M. H. Seavey: Solid State Commun.10, 219–223 (1972)
V. R. Gakel: Sov. Phys. JETP40, 908–915 (1975)
W. Rehwald, W. Wettling: Appl. Phys.22, 31–34 (1980)
J. E. Dikshtein, V. V. Tarasenko, V. G. Shavrov: Sov. Phys. JETP40, 404–407 (1975)
S. Iida, A. Tasaki: Proc. Int. Conf. on Magnetism (Nottingham 1964) pp. 583–588
E. A. Turov, V. G. Shavrov: Sov. Phys.-Solid State7, 166–172 (1965)
H. Dötsch: IEEE Trans. Mag.14, 692–694 (1978)
H. Dötsch, H. J. Schmitt, J. Müller: Appl. Phys. Lett.23, 639–641 (1973)