• Journal of the Korean Magnetics Society
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• v.4 no.2
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• pp.100-105
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• 1994

Ni-Fe thin films are deposited on the corning glass substrate by means of RF magnetron sputtering system In order to investigate the dependence of the prorerties of Ni-Fe thin films on the film thickness, ferromagnetic reson¬ance spectrum has been examined. The effective magnetization $M_{eff}$ is constant for all samples, while the exchange stiffness constant A increases with the film thickness. A tendency that spectroscopic splitting factor g increases with the sample thickness, we expect that the increase of the contribution of the orbital motion to the magnetic moment as a reason for it.

• Korean Journal of Materials Research
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• v.4 no.1
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• pp.117-124
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• 1994

The reduction of saturation magnetization in the Mg-Mn microwave ferrites was achieved by substituting the non-magnetic A1 ion for Fe ion. It is necessary for extending the operation frequencies that there is no change in other properties of the microwave ferrites. The electrical and magnetic properties are characterized where the composition of the ferrites studied was given by the general formula $(MgO)_{1.0}(MnO)_{0.1}(Al_xFe_{1.9-x}O_{2.85}$ with x ranging from 0.1 to 0.4. The saturation magnetization and the ferromagnetic resonance linewidth was decreased by the substituting amount of $Al_2O_3$. The value of coercive field was low enough over the composition of x=O.2 and the high squareness ratio was obtained all over the amount of substitution. It is feasible to select the proper application area with the combination of various properties ; that is, low coercive field, high squareness ratio, optimum saturation magnetization and ferromagnetic resonance linewidth.

• Journal of the Korean Magnetics Society
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• v.15 no.1
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• pp.25-29
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• 2005

Magnetic properties of YIG films grown by solid phase epitaxy (SPE) was measured as a function of temperature with focus on magneto-crystalline and perpendicular magnetic anisotropy. Perpendicular magnetic anisotropy was not induced in the SPE YIG films annealed at low temperature by relaxing residual stress through formation of dislocation. On the contrary the films annealed at high temperature showed perpendicular magnetic anisotropy which shows very low density of dislocation. Perpendicular magnetic anisotropy field decreased linearly up to a high temperature of $230^{\circ}C$ above which magneto-crystalline anisotropy disappeared. Coercivity also decreased linearly with temperature up 세 $230^{\circ}C$. Magneto-crystalline anisotropy of perpendicular anisotropy induced epitaxial (111) YIG films can be measured using $H_k=4K_1/3M_s$. Temperature behavior of initial susceptibility can be successfully explained by Hopkinson effects. Curie temperature of YIG films grown on GGG substrate with high paramagnetic susceptibility can be easily measured using the results.

• Journal of the Korean Ceramic Society
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• v.36 no.3
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• pp.293-300
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• 1999

고주파 마그네트론 스퍼터법을 이용한 YIG(yttrium iron garnet)박막 제조시 기판유형, 기판온도, 스퍼터전력, 스퍼터가스 등의 증착변수와 증착후 열처리 조건이 YIG 박막의 결정성, 화학조성, 미세구조 그리고 자기적 특성에 미치는 영향에 대하여 고찰하였다. 75$0^{\circ}C$ 이상의 온도에서 수행한 증착후 열처리에 의하여 비정질 박막이 결정화되었으며, 특히 GGG(gadolinium gallium garnet)기판 위에 제조된 박막은 강한 (111)우선배향성을 나타냈다. 박막조성은 스퍼터가스 내의 산소분율에 민감하게 영향을 받았으며, 산소분율이 20%인 스퍼터가스를 사용하여 제조된 박막은 Y2.88Fe3.84O12의 조성을 나타내었다. 증착후 열처리 온도가 90$0^{\circ}C$로부터 110$0^{\circ}C$로 증가함에 따라, GGG 기판위의 박막의 표면거칠기는 2.5nm에서 40nm로 증가하였으며, 보자력과 강자성 공명 선폭은 감소하였다.

• Journal of the Korean Institute of Telematics and Electronics A
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• v.32A no.1
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• pp.97-102
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• 1995

The ferromagnetic resonance properties of Mg ferrites which have various porosity grain size, and saturation magnetization are measured at one frequency. This allows a determination of the anisotropy field(Ha). The saturation magnetization multiplied by porosity is the resonance magnetic field. As the saturation magnetization increases, the linewidth decerases due to decrement of magnetic inhomogenity in sample. the porosity is a major factor broadening the linewidth for Mg ferrite when porosity is more thatn 6%, and the anisotropy field is dominant when porosity is less than 6%.

• Journal of the Korean Magnetics Society
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• v.8 no.6
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• pp.357-361
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• 1998

For CoZr/Ag/CoCr trilayered films deposited by DC and FR magnetron sputtering method, ferromagentic resonance experiments have been used to investigate the dependence of the exchange coupling between CoZr and CoCr layers separated by Ag layer on the thickness of the Ag layer. The coupling strength K increases with increasing Ag thickness up to 10 $\AA$ with a maximum value of 748 Oe, but oscillates with increasing Ag thickness in the range from 20 to 100 $\AA$. The coupling strength is positive for all samples. Hence, it seems that the exchange coupling between CoZr and CoCr layers separated by Ag layer is ferromagnetic.

• Journal of the Korean Ceramic Society
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• v.37 no.10
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• pp.1001-1007
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• 2000

스크린 프린트법으로 MMIC(Monolithic Microwave Integrated Circuit)용 YIG 후막을 제조하였고, YIG의 조성과 프린트 조건의 변화가 다결정 $Y_{3-x}$C $a_{x}$ F $e_{5-x}$Z $r_{x}$ $O_{12}$ (x=0~0.3) 후막의 미세구조 및 자기적 특성에 미치는 영향을 고찰하였다. $Ca^{2+}$와 Z $r^{4+}$ 의 치환 첨가량이 0.2인 $Y_{2.8}$ C $a_{0.2}$F $e_{4.8}$ Z $r_{0.2}$ $O_{12}$ 조성의 paste로 제조된 YIG 후막의 경우, 포화 자화값이 최대를 나타내었으며, 강자성 공명 흡수선 폭은 최소를 나타내었다. 또한, YIG 후막의 두께 및 소결 유지시간 등의 제조조건을 제어함에 따라 치밀화 및 자기 특성이 향상됨을 확인할 수 있었다.다.다.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.16 no.3
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• pp.238-246
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• 2003

We have performed the simulation of ferromagnetic resonance spectra on the exchange coupled bilayer thin films at perpendicular configuration. Variables considered in spectrum calculation were the interfacial exchange constants per unit area, the layer thickness, and the surface anisotropy constants. In case of antiferromagnetic coupling, variation of exchange constant gave a great effect to the absorption spectra of the low and the high magnetization layer. Variation of thickness in low magnetization layer did nt nearly influenced the resonated field of the high magnetization layer. Also, the increase of negative surface anisotropy increased the resonance field of the low and the high magnetization layer.

• Journal of the Korean Magnetics Society
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• v.13 no.6
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• pp.221-225
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• 2003

Effects of annealing temperature on the crystalline and magnetic properties of YIG films grown by solid phase epitaxy. The eptiaxy films were made by annealing Fe-Y-O amorphous films in the air at 550-1050 $^{\circ}C$ which were sputtered on GGG (111) substrates in a conventional rf sputtering system. Crystallization temperature of Fe-Y-O amorphous films on GGG (111) substrate was between 600 and 650 $^{\circ}C$ which is much lower than that Fe-Y-O powder prepared by sol-gel method. Excellent epitaxial growth of YIG films could be conformed by the facts that the diffraction intensity of YIG (888) plane was comparable with that of GGG (888) plane and full width at half maximum of YIG (888) rocking curve was smaller than 0.14$^{\circ}$ when films were annealed at 1050 $^{\circ}C$. It could be seen that it is necessary to anneal the films at higher temperature for an excellent epitaxy because lattice parameter of YIG films were smaller and the peak of YIG (888) plane is higher and narrower with increasing annealing temperature. Films annealed at higher temperature shows M-H loop with perpendicular anisotropy which was due to 0.15％ lattice mismatch between YIG and GGG.

• Journal of the Korean Ceramic Society
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• v.32 no.2
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• pp.163-170
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• 1995

Sample size effect on ferromagnetic resonance (FMR) in polycrystalline MgFe2O4 has been investigated. The signal intensity (SI), resonance field (Hres) and line width (ΔH) were found to increase proportionally to r3 with the increase of sample radius. The r3-depencence of SI means the complete penetration of rf-field into the sample, and the broadening of ΔH due to the sample size appears to be closely related to the amount of scattering sources like pores. Meanwhile, the values of Hres (0) and ΔH (0) obtained by extrapolating the data of Hres (r) and ΔH (r) measured at several sizes to r=0, were in good agreement with those calculated using the Schlomann's equations for internal field and ΔH, respectively. This result indicates that the discrepancy between the measured FMR parameters and those calculated by Schlomann's equation could be ascribed to the effect of sample size. Thus it is suggested that the size effect on FMR should be removed for the analysis of the FMR parameters. Meanwhile, our result for the size dependance of ΔH was found to be contradictory to those reported by Dionne, where ΔH 1/r at a given surface roughness. This discrepancy appears to arise from the difference in the definition of reading the line width.