Fig. 5: Dynamic properties of the magnetostriction in NSMM with stripe domain.
From: Role of magnetostriction on power losses in nanocrystalline soft magnets
Snapshots of the motion of the stripe domain in the NSMM at (a) 37.5 ns, (b) 40.0 ns, and (c) 42.5 ns. d Oscillations of the magnetization and the external fields in the x1-direction. The blue curve represents the results with \(\lambda _{100}^\prime = 20.0 \times 10^{ - 5}\) and \(\lambda _{111}^\prime = - 7.22 \times 10^{ - 5}\), where \(\bar \xi _{11} = 0\), while the red curve represents the results for isotropic magnetostriction with \(\lambda _{100}^\prime = \lambda _{111}^\prime = 20.0 \times 10^{ - 5}\). The oscillating magnetic field is indicated by the dotted curve. e \(\bar \xi _{11}\) dependence of the phase differences between the external field and the domain motion. f \(\bar \xi _{11}\) dependence of the oscillation amplitudes of the domain wall motion. g \(\bar \xi _{11}\) dependence of the excess losses. In (e–g), blue and red colors represent the results for zero \(\bar \xi _{11}\) (\(\lambda _{111}^\prime = - 0.36\lambda _{100}^\prime\)) and isotropic magnetostriction (\(\lambda _{111}^\prime = \lambda _{100}^\prime\)), respectively.
