Ferromagnetic resonance and antiresonance in a composite material with cobalt nanoparticles

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Resumo

The frequency and field dependences of the wave transmission and reflection coefficients of a composite material with cobalt nanoparticles in an opal matrix were measured at frequencies of 26–38 GHz. The phenomena of ferromagnetic resonance and antiresonance have been experimentally studied. The theoretical calculation of the dependences of the transmission and reflection coefficients on the magnetic field is performed. The specificity of antiresonance in a composite material has been revealed. The importance of taking into account the interference of waves in the nanocomposite is indicated. The field dependence of the depth of penetration of microwaves into the composite is calculated. Formulas for calculating the antiresonance field in a composite material are obtained.

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Sobre autores

O. Nemytova

Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences

Email: rin@imp.uran.ru
Rússia, Ekaterinburg, 620108

D. Perov

Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences

Email: rin@imp.uran.ru
Rússia, Ekaterinburg, 620108

E. Kuznetsov

Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences

Email: rin@imp.uran.ru
Rússia, Ekaterinburg, 620108

A. Rinkevich

Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences

Autor responsável pela correspondência
Email: rin@imp.uran.ru
Rússia, Ekaterinburg, 620108

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2. Fig. 1. SEM image of the structure obtained at 150,000 magnification (a) and EDAX spectrum (b) for a sample of nanocomposite with Co particles.

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3. Fig. 2. X-ray diffraction pattern of a nanocomposite sample based on an opal matrix with metallic Co particles in interspherical voids.

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4. Fig. 3. Magnetization curve of the composite measured at T = 2 K and hysteresis loops at T = 300 K and T = 2 K.

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5. Fig. 4. Scheme of microwave measurements. Shaded area – nanocomposite sample, H – external constant magnetic field, H~ – intensity of alternating microwave magnetic field, E~ – intensity of alternating microwave electric field, k – wave vector of electromagnetic wave.

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6. Fig. 5. Experimental (dashed lines and empty symbols) and theoretical (solid lines and filled symbols) dependences of relative changes in the transmission (a) and reflection (b) coefficients on the magnetic field for a sample based on an opal matrix with metallic Co particles in the interspherical voids.

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7. Fig. 6. Results of calculating the field dependence of the real (filled symbols) and imaginary (empty symbols) parts of the effective magnetic permeability (a); theoretical (solid lines and filled symbols) and experimental (dashed lines and empty symbols) field dependences of the dissipation parameter (b).

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8. Fig. 7. Dependences of real (filled symbols) and imaginary (empty symbols) parts of the wave number on the magnetic field.

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9. Fig. 8. Results of calculating the field dependence of the penetration depth of microwaves into the nanocomposite.

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10. Fig. 9. Field dependences of the ratio of sample thickness to wavelength in a composite for different frequencies.

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