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| Content Provider | IEEE Xplore Digital Library |
|---|---|
| Author | Kondo, K. Chiba, T. Yoshida, S. Okamoto, S. Shimada, Y. Matsushita, N. Abe, M. |
| Copyright Year | 1965 |
| Abstract | We previously revealed that spin sprayed Ni-Zn ferrite films had a weak in-plane uniaxial magnetic anisotropy induced parallel to the liquid flow direction during the spin spraying. Adding a small amount of Co to the films, we made the uniaxial magnetic anisotropy definitely strong. The imaginary part of the complex permeability (/spl mu/=/spl mu/'-j/spl mu/'') of the Co-containing films measured in the remanence state exhibited a dual step-like dispersion. In order to reveal the influence of magnetic anisotropy of the films on the magnetic resonance, we deposited, in this study, films #1 (Ni/sub 0.17/Zn/sub 0.22/Fe/sub 2.61/O/sub 4/) and #2 (Ni/sub 0.19/Zn/sub 0.20/Co/sub 0.03/Fe/sub 2.58/O/sub 4/) by spin spray ferrite plating at 90/spl deg/C. The imaginary permeability in the remanence state of the film #1 (which exhibited no definite in-plane magnetic anisotropy) had a maximum at about 450 MHz, which increased with increasing external dc magnetic field, H/sub dc/ in the range of 1-3 GHz to give a similar spectrum to that of the film #2. The resonance field, H/sub R/ of the film #2 under H/sub dc/ of 1-2 kOe, which was strong enough to saturate the magnetization, exhibited a prominent in-plane angular dependence, while H/sub R/ of the film #1 exhibited a very weak angular dependence. The difference between the maximum and the minimum values of H/sub R/ for the film #2 was about 60 Oe. This means that the film #2 consists of two regions, one with a crystalline anisotropy field having an in-plane isotropic distribution due to the cubic spinel structure, and the other with an induced uniaxial anisotropy field, H/sub k/ of about 60 Oe. Assigning H/sub k/ of 60 Oe, we calculated the natural resonance frequency, f/sub r/ as 1.6 GHz. This value approximately coincided with that of the higher frequency step of /spl mu/'' for the film #2 in the remanence state. This suggests that the magnetic loss in the remanence state for the films like #2 (which exhibit prominent uniaxial anisotropy induced in film plane) is ascribed to the two regions described above. |
| Sponsorship | IEEE Magnetics Society |
| Starting Page | 3463 |
| Ending Page | 3465 |
| Page Count | 3 |
| File Size | 165390 |
| File Format | |
| ISSN | 00189464 |
| Volume Number | 41 |
| Issue Number | 10 |
| Language | English |
| Publisher | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Publisher Date | 2005-10-01 |
| Publisher Place | U.S.A. |
| Access Restriction | One Nation One Subscription (ONOS) |
| Rights Holder | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Subject Keyword | Magnetic resonance Ferrite films Permeability Magnetic films Magnetic anisotropy Remanence Spraying Anisotropic magnetoresistance Zinc Iron Ni-Zn(-Co) ferrite film Complex permeability ferrite plating ferromagnetic resonance (FMR) |
| Content Type | Text |
| Resource Type | Article |
| Subject | Electronic, Optical and Magnetic Materials Electrical and Electronic Engineering |
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