• Journal of the Korean Magnetics Society
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• v.25 no.5
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• pp.144-148
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• 2015

We grew spinel structured $CoMn_2O_4$ thin films and have studied post-growth annealing effects on their physical properties. After post-growth annealing at $700^{\circ}C$ that is lower than the growth temperature ($720^{\circ}C$), crystal structure became cleared accompanying a change of surface structure. In the temperature dependences of magnetization, phase transitions were observed at ~100 K for both before and after post-growth treated samples which were not observed for the bulk. For both samples, ferromagnetic behaviors were observed above 100 K while it turned to ferrimagnetism at low temperature below 100 K. In particular, the ferrimagnetic behavior became strong after the post-growth treatment. These results indicate that the post-growth annealing process plays an important role in determining the physical properties of spinel $CoMn_2O_4$ thin film.

• Proceedings of the Korean Magnestics Society Conference
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• 2009.05a
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• pp.236-236
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• 2009

• Proceedings of the Korean Magnestics Society Conference
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• 2001.10a
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• pp.52-53
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• 2001

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 1998.06a
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• pp.49-52
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• 1998

Preparation of hexagonal strontium-ferrite by modified spray co-roasting(MSC:H) which is expected to shorkn the length of the process and to elevate the magnetic properties of hard ferrite was studied. We prapared $Fe_2O_3/SrCO_3$ mixture powders by MSCR after stirring ionized $FeCI_2$ in distilled water with solid state $SrCO_3$. And then calcined the mixture powders up to $1150^{\circ}C$ for Sr-ferrite powders It is possible to prepare hexaferrite powders with high saturation magnetization (Ms > 69 emu/g) , coercivity (Hc > 4000 Oe) The nlagnetic values of saturation magnetization iire higher than those achieved by the conventional technique.

• Electronics and Telecommunications Trends
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• v.18 no.6 s.84
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• pp.41-48
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• 2003

본 논문은 아이솔레이터의 소재 파라미터에 의한 삽입손실 영향에 대하여 서술하였다. 본 논문에서는 페리자성공명반치폭($\Delta$Η), 유전손실, 자계세기 그리고 포화자화에 대한 아이솔레이터 삽입손실의 관계를 알아 보았고, 또한 공진 아래 모드를 사용한 아이솔레이터의 온도안정화 연구 및 구조설계에 대하여알아 보았다. 아이솔레이터의 온도특성은 영구자석, YIG(Yttium Iron Garnet) 페라이트 그리고 공진기로사용되는 도체 등에 의한 변화에 대하여 본 논문에서는 실험시제품을 제작하여 측정 분석하였다. 측정결과 시뮬레이션 결과와 실험시제품 측정결과가 거의 일치하는 것을 알 수 있었다. 삽입손실 0.18~0.24dB, 반사손실 27dB, 아이솔레이션 27dB 그리고 대역폭 500MHz를 얻을 수 있었다. 이때 실험에 사용한 소재 파라미터는 포화자화 550G, 유전손실, $0.0004\Delta$Η20, 유전율 14로 하였다. 또한 온도안정화실험에서는 구조를 개선하여 온도안정화를 이루었다.

• Proceedings of the Korean Magnestics Society Conference
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• 2003.06a
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• pp.192-193
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• 2003

YIG 에피택시박막은 다른 강자성, 페리자성재료에 비해 수 GHz의 영역에서 매우 우수한 특성을 나타내고 있다. YIG 에피택시 박막은 고상에피택시 방법으로 제조할 경우 매우 편리하게 제조할 수 있는 것으로 알려져 있는데, 이 방법은 상온에서 Y-Fe-O 박막을 GGG(111)기판에 스파터한 뒤 공기 중에서 열처리하면 간편하게 얻을 수 있다. 이 방법은 통상과 같이 고온에서 아주 느린 속도로 에피택시박막을 성장시키는 스파터방법에 비해 매우 간편하고 경제적인 것으로, 본 연구에서는 보통의 분말소결공정으로 제작된 2.5인치 YIG 타겟을 사용하여 두께 2.5 $\mu\textrm{m}$ 비정질 Fe-Y-O 박막을 만든 뒤 550 - 1050 $^{\circ}C$의 공기 중에서 열처리하였다. 비정질 박막을 $600^{\circ}C$이하에서 10 시간동안 열처리하였을 경우 매우 약한 YIG상의 회절선만 관찰할 수 있었다. 반면에 온도를 $650^{\circ}C$로 올리면 매우 강한 (444) 또는 (888)회절선과 매우 약한 다른 회절선을 관찰 할 수 있었다. 이 시편의 경우 (888)회절선의 강도는 GGG기판의 (888)회절선의 강도와 비교할 정도로 매우 강하여 에피택시성장이 매우 잘 이루어질 수 있다는 가능성을 확인할 수 있었다. 그리고 YIG(888) 회절선의 록킹곡선의 반가폭이 0.14$^{\circ}$ 이었고, 이것은 에피택시성장이 매우 잘 이루어지고 있음을 의미하는 것이다. 열처리 온도가 감소함에 따라 YIG박막의 격자상수는 감소하였으며 YIG(888)회절선의 강도는 그림 1과 같이 넓어지고 그 강도는 약해진다.

• The Journal of Korean Institute of Communications and Information Sciences
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• v.22 no.11
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• pp.2573-2584
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• 1997

In this paper, Ca, Sn substitute YIC(Yttrium Iron Garnet) ceramics were fabricated with Al substitutions in Fe sites. The strip-line circulator was designed and the properties of fabricated ciculator were measured. When the electric, magnetic and microwave properties were measured in Ca, Sn substituted YIG with Al subsititions, the relative permittivity and perfmeability in microwave frequencies were 15.623 and 0.972, repectively. For $Y_{2.4}Ca_{0.3}Sn_{0.3}Fe_{5-x}Al_xO_{12}$ garnet ceramics sintered at $1450^{\circ}C$, the ferrimagnetic resonance line width $\Delta{H}$) of 42 Oe and the saturation magnetization of 487 G were measured at 10 GHz. The strip-line circulator was simulated with 3-D FEM(Finite Element Method) software and designed to have insertion loss of 0.8dB, return loss of 25dB, isolation of 35dB at the center frequency of 1.9GHz. The fabricated strition loss of 0.8B, reture loss of 25dB, isolation of 35dB at the center frequency of 1.9GHz. The fabricated strip-line junction circulator using above YIG ceramics had insertion loss of 0.869dB, return loss of 26.955dB, isolation of 44.409dB at the center frequency of 1.9GHz.

• Korean Journal of Materials Research
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• v.5 no.2
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• pp.239-245
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• 1995

Mn-Zn ferrite thin films were deposited on $SiO_2(1000 \AA)/Si(100)$ by ion beam sputtering using a single ion source. A mosaic target consisting of a single crystal(ll0) Mn-Zn ferrite with a Fe metal strip on it was used. As-deposited films without oxygen gas flow have a wiistite structure due to oxygen deficiencies, which originated from the extra metal atoms sputtered from the metal strips during deposition. The as-deposited films with oxygen gas flow, however, have a spinel structure with (111) preferred orientation. The crystallization of thin films was maximized at the ion beam extraction voltage of 2.lkV, at which the deposited films are bombarded appropriately by the energetic secondary ions reflected from the target. As the extraction voltage increased or decreased from the optimum value, the crystallinity of thin films becomes poor owing to a weak and severe bombardment of the secondary ions, respectively. Crystallization due to the bombardment of the secondary ions was also maximized at the beam incidence angle of $55^{\circ}$. The as-deposited ferrite thin films with a spinel structure showed ferrimagnetism and had an in-plane magnetization easy axis.

• Journal of the Korean Magnetics Society
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• v.13 no.3
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• pp.97-102
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• 2003

Synthetic ferrimagnetic layer (SyFL) with structure NiFe/Ru/NiFe which can be applied high density TMR device in free layer were prepared by an inductively coupled plasma (ICP) helicon-sputter. We proposed a model of predicting coercivity (H$\_$c/), spin-flopping field (H$\_$sf/), and saturation field (H$\_$s/) as a function of Ru thicknesses, from the equilibrium state of energies of Zeeman, exchange, and uniaxial anisotropy. We fabricated the samples of Ta(50 ${\AA}$)/NiFe(50${\AA}$)nu(4∼20${\AA}$)NiFe(30 ${\AA}$)/Ta(50${\AA}$), and measured the M-H loops with a superconduction quantum interference device (SQUID) applying the external field up to ${\pm}$ 15 kOe. The result was well agreed with the proposed model, and reveal K$\_$u = 1000 erg/㎤, J$\_$ex/ =0.7 erg/$\textrm{cm}^2$. We report that H$\_$c/ below 10 Oe is available, and R$\_$u/ thickness range should be in 4-10 ${\AA}$ for MRAM application. Our result implies that permalloy layers may lead to considerable magnetostriction effect in SyFL and intermixing in NiFe/Ru interfaces.

• Journal of the Korean Magnetics Society
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• v.22 no.1
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• pp.19-22
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• 2012

$Ba_2Mg_{0.5}Co_{1.5}(Fe_{0.99}In_{0.01})_{12}O_{22}$ was prepared by the conventional solid-state reaction method, and studied by x-ray diffractometer, vibrating sample magnetometer, and Mossbauer spectrometer. The crystal structure was determined to be a single-phased rhombohedral with space group R-3m. Magnetization value were $M_s$ = 28.6 emu/g at 295 K. The hysteresis loops indicate that all the samples are ferrimagnetic behaviors. Mossbauer spectra of $Ba_2Mg_{0.5}Co_{1.5}(Fe_{0.99}In_{0.01})_{12}O_{22}$ have been 6-sextet taken at various temperatures ranging from 4.2 to 620 K. Based on the isomer shift (${\delta}$) values of all samples, the charge states were found to be $Fe^{3+}$ state at all temperatures, the Curie temperature was determined to be 630 K by the ZVC curve.