1993
DOI: 10.1063/1.353259
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Frequency-dependent complex permeability in rare earth-substituted cobalt/nonmagnetic transition metal soft ferromagnetic amorphous thin films

Abstract: Frequency and field dependence of magnetoelectric interactions in layered ferromagnetic transition metalpiezoelectric lead zirconate titanate Appl. Phys. Lett. 87, 222507 (2005); 10.1063/1.2137450 Fluctuation field and time dependence of magnetization in TbFeCo amorphous rare earth-transition metal thin films for perpendicular magnetic recording A study of complex permeability in rare earthsubstituted cobalt/nonmagnetic transition metal amorphous thin films J. Appl. Phys. 73, 5592 (1993); 10.1063/1.353661 Micr… Show more

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Cited by 33 publications
(11 citation statements)
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“…It can be seen that in a wide x range, good high-frequency properties are obtained for (Ni 75 Fe 25 ) x (ZnO) 1−x films, suggesting that excellent high-frequency properties may be realized in other MSCGF systems, such as FeCo-SnO 2 , etc. For the typical sample with x = 0.74, it is seen that the μ is more than 200 below 1.0 GHz, while the imaginary part μ is much smaller than μ when f < 1.0 GHz and gradually increases to a maximum at f = 1.32 GHz which can be ascribed to the ferromagnetic resonance FMR [15] The experimental curves were fitted with formulas (2)-(4) quite well as shown by the solid lines. For the sample with x = 0.74, 4πM s = 7900 Gs and H k = 26 Oe, according to formula (4), the FMR frequency f r is approximately 1.30 GHz, consistent with the experiment result.…”
Section: Resultsmentioning
confidence: 91%
“…It can be seen that in a wide x range, good high-frequency properties are obtained for (Ni 75 Fe 25 ) x (ZnO) 1−x films, suggesting that excellent high-frequency properties may be realized in other MSCGF systems, such as FeCo-SnO 2 , etc. For the typical sample with x = 0.74, it is seen that the μ is more than 200 below 1.0 GHz, while the imaginary part μ is much smaller than μ when f < 1.0 GHz and gradually increases to a maximum at f = 1.32 GHz which can be ascribed to the ferromagnetic resonance FMR [15] The experimental curves were fitted with formulas (2)-(4) quite well as shown by the solid lines. For the sample with x = 0.74, 4πM s = 7900 Gs and H k = 26 Oe, according to formula (4), the FMR frequency f r is approximately 1.30 GHz, consistent with the experiment result.…”
Section: Resultsmentioning
confidence: 91%
“…It is seen from Fig. 5 (a) that for this film is more than 140 below 1.5 GHz, then gradually decreases with frequency, while the imaginary part gradually increases to a maximum at f = 2.6 GHz, which can be ascribed to the ferromagnetic resonance (FMR) [11]. The measured curves ∼ f data were fitted well with the solution of Landau-Lifshitz equations taking account of the coherent spin procession [12,13], as shown by the solid lines in Fig.…”
Section: Resultsmentioning
confidence: 91%
“…The other researchers showed that the magnetization dynamics of soft ferromagnetic Ni 81 Fe 19 thin films at frequencies above 1 GHz can be tuned using rare-earth dopant while retaining the important soft magnetic properties [8,9]. Moreover, an appreciable increase of damping factors was reported due to rare-earth elements addition in the publications [7][8][9].…”
Section: Introductionmentioning
confidence: 94%
“…On the other hand, Russat Ideally such doping increases the frequency response without affecting the soft magnetic properties of the films [7]. The other researchers showed that the magnetization dynamics of soft ferromagnetic Ni 81 Fe 19 thin films at frequencies above 1 GHz can be tuned using rare-earth dopant while retaining the important soft magnetic properties [8,9].…”
Section: Introductionmentioning
confidence: 98%