• Proceedings of the Materials Research Society of Korea Conference
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• 2003.03a
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• pp.176-176
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• 2003

강자성 반도체(DMS)는 반도체에 전이금속을 doping함으로써 반도체의 전자 수송 특성과 전이 금속 이온에 의한 자기적 특성을 동시에 발현할 수 있도록 설계된 물질로서 '스핀 전자공학'의 구현을 위해 현재 활발히 연구되고 있는 분야이다. 특히 높은 전기 전도도와 투명 광 특성을 가지는 ZnO계는 전이금속을 첨가 할 경우 상온에서도 강자성 특성을 보일 것이라는 연구가 발표 된 이후 큰 주목을 받고 있으며, 실제로 Tc가 상온 이상인 결과들이 최근 발표되고 있다. 그러나 PLD에 의해 증착 된 Co-doped ZnO 경우 강자성 물성의 재현성이 아주 낮은 것으로 알려져 있는 둥 강자성 발현의 기원이 아직도 명확히 규명되지 못한 상태이다. 이에 본 연구에서는 Co-doped ZnO 계의 강자성 발현의 기원을 밝히고자 고상 반응법을 이용하여 다결정계를 제조한 후 X-선 회절 분석과 Raman 분광법을 이용하여 제2차상의 존재 유무 및 Co 이온의 치환 정도를 분석하였다. 다음으로 방사광 EXAFS 분석을 행하여 ZnO내에서의 Co 이온의 원자가 상태를 분석하고, PPMS를 사용 M-T curve를 측정/분석함으로써 강자성 발현의 기원을 규명하고자 하였다.

• Journal of the Computational Structural Engineering Institute of Korea
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• v.15 no.4
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• pp.727-739
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• 2002

Based on a generalized variational principle for magneto-thermo-elasticity, a theoretical model is proposed to describe the coupled magneto-thermo-elastic interaction in soft ferromagnetic plates. Using the linearized theory of magneto-elasticity and perturbation technique, we analyze the magneto-elastic and magneto-thermo-elastic instability of simply supported ferromagnetic plates subjected to thermal and magnetic fields. A nonlinear finite element procedure is developed next to simulate the magneto-thermo-elastic behavior of a finite-size ferromagnetic plates. The effects of thermal and magnetic fields on the magneto-thermo-elastic bending and buckling is investigated in some detail.

• Proceedings of the Korean Magnestics Society Conference
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• 2002.12a
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• pp.74-75
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• 2002

교환바이어스(exchange bias)현상은 강자성과 반강자성의 접합계면에서 강한 상호교환결합력 (exchange force)에 의해 발생하는 것으로 알려져 왔다. 이 현상은 1956년 Meiklejohn과 Bean에 의해 CoO층으로 둘러 쌓인 Co입자에서 발견된 이후[1], 강자성과 반강자성의 접합계면을 가지는 다층박막에서의 교환바이어스에 대한 연구가 진행되어왔다[2-6]. 이는 강자성/반강자성박막의 교환바이어스 특성을 이용하여, 강자성 박막의 스핀방향을 고정시킬 수 있기 때문이다. (중략)

• Composites Research
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• v.23 no.1
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• pp.51-53
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• 2010

자기장하에서 액체 성질인 유동성과 고체 성질인 자성을 갖는 강자성/자기흐름 유체의 제조방법, 강자성/자기흐름 유체의 조성 및 미세구조와 유체 매트릭스의 구조에 따른 자기특성과 강자성/자기흐름 유체의 물리적, 기계적 성질을 조사하고 최근 연구개발되고 있는 전기흐름유체(electrorheological fluid)의 특성과 비교하였으며, 또한 이를 바탕으로 방탄복에 대한 적용성을 검토하였다.

• Journal of the Korean Magnetics Society
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• v.22 no.2
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• pp.66-72
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• 2012

The findings of ferromagnetic superconductor have attracted much attention not only for fundamental research to investigate how the antagonistic properties of ferromagnetism and superconductivity coexist peacefully but also for potential technological applications. Firstly, in order to help for understanding the ferromagnetic superconductor, I have explained the orbital and paramagnetic pair-breaking effects of magnetic field, which breaks the superconducting Cooper pairs. In addition to such effects of magnetic field, the singlet Cooper pairs become unstable upon going through the ferromagnetic materials by the proximity effect. The proximity effect occurs at the interface of thin films composing of superconductor and ferromagnet and leads to have very short penetration depth of Cooper pairs. However, a type of odd-frequency triplet in comparison with the singlet could be very stable and has a longer effective depth. It needs to be explored for the innovative spintronic devices. Finally, various ferromagnetic superconductors coexist and the lower-dimensional materials under the Quantum confinement effect have been introduced.

• Journal of the Korean Magnetics Society
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• v.24 no.1
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• pp.11-17
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• 2014

We measured the ferromagnetic resonance (FMR) signal using the monodisperse iron oxide nanoparticles with size D=4.67 nm, 5.64 nm and 6.34 nm synthesized by using the thermal decomposition method, respectively. The measured ferromagnetic resonance signals were compared with the calculated ones for superparamagnetic nanoparticles with lognormal volume distribution. The FMR linewidth broadening was propositional to tanh($V^2$), where V was volume of nanoparticles. The narrow linewidth of small size nanoparticles was due to the surface spins, while the broad linewidth of large size nanoparticles was due to the bulk spins affected by the crystalline structure of iron oxide nanoparticles. The superposition of surface and bulk effect was confirmed at D=5.64 nm nanoparticles, which was near the critical size for linewidth transition from surface effect to bulk effect.

• Journal of the Korean Magnetics Society
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• v.27 no.3
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• pp.77-81
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• 2017

The rotatable anisotropy effect was observed in the ferromagnetic resonance measurement in exchange coupled ferromagnetic/antiferromagnetic thin films and it was due to rotation of antiferromagnetic layer by the exchange coupling energy. We analyzed the CoFe thickness dependence of rotatable anisotropy field and ferromagnetic resonance linewidth in exchange coupled $CoFe(t_F)/MnIr(2.5nm)$ thin films. The rotatable anisotropy field was inversely propositional to the CoFe thickness and it was well fitted by the rotatable anisotropy energy of $0.96erg/cm^2$. The ferromagnetic resonance linewidth were linearly propositional to the rotatable anisotropy field in $t_F$ < 50 nm, while it was more dominated by the eddy current effect in $t_F$ > 50 nm.

• Proceedings of the Materials Research Society of Korea Conference
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• 2003.03a
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• pp.178-178
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• 2003

II-Ⅵ족 반도체 중에서 넓은 밴드갭을 가지는 ZnO에 Mn 이온을 doping할 경우 Tc가 상온보다 높을 것이라는 이론적 계산이 2000년 Science에 발표되었다. 이후 ZnO에 전이금속 이온을 doping하여 상온에서도 강자성을 나타내는 자성 반도체 (DMS)를 만들기 위한 연구가 활발히 진행되고 있다. Co-doped ZnO 박막은 PLD로 증착하였을 경우 Tc가 상온보다 높으나 재현성이 낮은 것으로 알려져 있었다. 그러나 최근 sol-gel 방법을 이용하여 Co-doped ZnO 박막을 제조하면 강자기 특성의 재현성을 높일 수 있다는 결과가 보고되었다. 이에 본 연구에서는 sol-gel 방법을 사용하여 여러 조성의 Co-doped ZnO 박막을 합성한 후 이들의 자성 특성을 검토하였다. 이러한 결과를 바탕으로 Co-doped ZnO 박막에서 강자성 발현의 근원을 규명하고자 (ⅰ) 조성에 따른 Co-doped ZnO의 Raman peak과 EXAFS peak의 변화를 측정하여 구조적 특성과 ZnO 내에서의 Co 이온의 상태를 분석하였으며, (ⅱ) Hall 효과 실험으로 carrier density를 측정함으로써 Fermi 준위에서의 파수 벡터의 크기를 산출하고자 하였다.

• Journal of the Korean Magnetics Society
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• v.23 no.2
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• pp.37-42
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• 2013

The out-of-plane and in-plane angular dependence of ferromagnetic resonance field was measured in NiFe thin films fabricated by magnetron sputtering. The effective magnetization was obtained from the out-of-plane angular dependence of ferromagnetic resonance field, which was well agreed with calculated one. The decrease of effective magnetization with NiFe thickness was due to the surface anisotropy constant of $K_s=-0.23\;erg/cm^2$. The in-plane uniaxial anisotropy fields were obtained from the in-plane angular dependence of ferromagnetic resonance field. The easy axis of in-plane uniaxial anisotropy field was rotated to the reverse direction of applied magnetic field during sample fabrication, which was explained by the antiferromagnetic NiFeO layer at sample surface.

• Journal of the Korean Magnetics Society
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• v.24 no.6
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• pp.165-170
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• 2014

We analyzed the ferromagnetic and spin wave resonance signals measured in amorphous CoFeB thin films with different thickness. The ferromagnetic resonance field ($H_{FMR}$) was not depend on the thickness of CoFeB films, but the spin wave resonance field ($H_{SWR}$) was well fitted with the theoretical prediction depending on the thickness. The uniaxial anisotropy field of $H_k$ = 37 Oe was obtained from the angular dependent $H_{FMR}$ in CoFeB films. The $H_{SWR}$ showed same angular behaviors with $H_{FMR}$, however, the amplitude of spin wave resonance signals showed 5.7 times higher than that of ferromagnetic resonance signals in CoFeB film with t = 100 nm. The higher signals were due to the two reasons; one was the small damping for the spin wave propagation without degradation, the other was uniform magnetization for the ideal standing wave modes.