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J. Appl. Phys. 107, 053905 (2010); doi:10.1063/1.3313920 (18 pages)
Present status of theoretical modeling the magnetoelectric effect in magnetostrictive-piezoelectric nanostructures. Part II: Magnetic and magnetoacoustic resonance ranges
(Received 30 April 2009; accepted 18 January 2010; published online 4 March 2010)
© 2010 American Institute of Physics
Article Outline
- INTRODUCTION
- Influence of a constant electric field on magnetic susceptibility
- Calculation of ME coefficients
- Two-layer structure (bimorph)
- General theory: Macroscopic homogeneous model
- Contribution of flexural deformations and effect of substrate clamping
- ME susceptibility of ferrite-ferroelectric composites
- Enhancement in ME coupling in MAR region
- Bias field perpendicular to sample plane
- Tangentially magnetized film
- Effects of exchange interactions on MAR
- Electric field induced magnetic excitations
- CONCLUSIONS
EDITORIALLY RELATED
- Present status of theoretical modeling the magnetoelectric effect in magnetostrictive-piezoelectric nanostructures. Part I: Low frequency and electromechanical resonance ranges
M. I. Bichurin et al.
J. Appl. Phys. 107, 053904 (2010)JAPIAU000107000005053904000001
RELATED DATABASES
KEYWORDS and PACS
Keywords
elasticity, ferrites, ferromagnetic resonance, lead compounds, lithium compounds, magnetoacoustic resonance, magnetoelastic effects, magnetoelectric effects, magnetostriction, nanostructured materials, nickel compounds, piezoelectric materials, yttrium compounds
PACS
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Magnetoelectric effects, multiferroics
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Nanocrystalline materials
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Piezoelectricity and electromechanical effects
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Magnetomechanical effects, magnetostriction
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Ferrimagnetics
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Ferromagnetic, antiferromagnetic, and ferrimagnetic resonances; spin-wave resonance
ARTICLE DATA
PUBLICATION DATA
Publisher:
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