• Proceedings of the Materials Research Society of Korea Conference
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• 2003.11a
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• pp.237-237
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• 2003

교환바이어스(exchange bias)현상은 강자성과 반강자성의 접합계면에서 강한 상호 교환결합력에 의해 발생하는 것으로 알려져 있다. 이 현상은 1956년 Meiklejohn과 Bean에 의해 CoO층으로 둘러싸인 Co 입자에서 발견된 이후[1], 강자성과 반강자성의 접합계면을 가지는 다층박막에서의 교환바이어스에 대한 연구가 진행되어왔다[2-6]. 이는 강자성/반강자성 박막의 교환바이어스 특성을 이용하여, 강자성 박막의 스핀방향을 고정시킬 수 있기 때문이다. 이러한 교환바이어스 특성은 하드드라이브의 고밀도 자기헤드소자 및 비휘발성 자기메모리소자에 응용되어지는 등 경제적 가치를 갖는 기술적인 면과 교환바이어스라는 자기특성의 학문적인 가치로 인해 이 분야에 대한 집중적인 투자와 연구가 이루어지고 있다. 최근에는 교환바이어스 현상의 원인과 형성기구에 대한 연구가 활발히 진행되고 있다. 그러나 강자성과 반강자성 박막의 단거리 상호 교환결합력에 의한 교환바이어스 현상은, 계면의 원자구조, 자기구조 및 각자성층의 여러 가지 인자들에 대해서 지속적으로 연구되고 있다.

• Journal of the Korean Magnetics Society
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• v.26 no.1
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• pp.1-6
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• 2016

Pd has the highest magnetic susceptibility among single element metals and often shows ferromagnetism under some special environments. In this paper, we report magnetism of 5- and 9-monolayers (ML) calculated by using full-potential linearized augmented plane wave method. Exchange-correlation interaction is taken into account in local density approximation (LDA) and generalized gradient approximation (GGA) and calculational results in LDA and GGA are compared with each other. It is found that calculations by LDA are more reliable compared to those by GGA because LDA prediction of paramagnetism of bulk Pd is consistent with experiments, whereas GGA predicts wrongly ferromagnetim of bulk Pd. Calculational results in LDA on a 5-ML Pd(111) thin film shows a ferromagnetic ground state unlike a paramagnetic ground state of bulk Pd. The center Pd layer of the 5-ML Pd(111) thin film has the largest magnetic moment ($0.273{\mu}_B$) among the layers and |m| = 1 orbital states play a dominant role in stabilizing the ferromagnetism of the 5-ML Pd(111) thin film. A 9-ML Pd(111) thin film in a ferromagnetic state has almost the same total energy as in a paramagnetic state. Since the magnetization of the 9-ML Pd(111) thin film is stable, the ferromagnetic state may be meta-stable.

• Journal of the Korean Society for Nondestructive Testing
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• v.36 no.6
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• pp.483-489
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• 2016

The typical methods used for inspecting ferromagnetic pipes include the ultrasonic testing (UT) contact method and the following non-contact methods: magnetic flux leakage (MFL), electromagnetic acoustic transducers (EMAT), and remote field eddy current testing (RFECT). Among these methods, the RFECT method has the advantage of being able to establish a system smaller than the diameter of a pipe. However, the method has several disadvantages as well, including different sensitivities and difficult-to-repair coil sensors which comprise its array system. Therefore, a giant magneto-resistance (GMR) sensor was applied to address these issues. The GMR sensor is small, easy to replace, and has uniform sensitivity. In this experiment, the GMR sensor was used to measure remote field and defect signal characteristics (in the axial and radial directions) in a ferromagnetic pipe. These characteristics were measured in an effort to investigate standard defects at changing depths within a pipe. The results show that the experiment successfully demonstrated the applicability of the GMR sensor to RFECT signal detection in ferromagnetic pipe.

• Proceedings of the Materials Research Society of Korea Conference
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• 2003.11a
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• pp.236-236
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• 2003

교환바이어스(exchange bias)현상은 강자성과 반강자성의 접합계면에서 강한 상호 교환결합력에 의해 발생하는 것으로 알려져 있다. 이 현상은 1956년 Meiklejohn과 Bean에 의해 CoO층으로 둘러싸인 Co 입자에서 발견된 이후[l], 강자성과 반강자성의 접합계면을 가지는 다층박막에서의 교환바이어스에 대한 연구가 진행되어왔다[2-6]. 이는 강자성/반강자성 박막의 교환바이어스 특성을 이용하여, 강자성 박막의 스핀방향을 고정시킬 수 있기 때문이다. 이러한 교환바이어스 특성은 하드드라이브의 고밀도 자기헤드소자 및 비휘발성 자기메모리소자에 응용되어지는 등 경제적 가치를 갖는 기술적인 면과 교환바이어스라는 자기특성의 학문적인 가치로 인해 이 분야에 대한 집중적인 투자와 연구가 이루어지고 있다. 최근에는 교환바이어스 현상의 원인과 형성기구에 대한 연구가 활발히 진행되고 있다. 그러나 강자성과 반강자성 박막의 단거리 상호 교환결합력에 의한 교환바이어스 현상은, 계면의 원자구조, 자기구조 및 각자성층의 여러 가지 인자들에 대해서 지속적으로 연구되고 있다.

• Proceedings of the Korean Magnestics Society Conference
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• 2010.06a
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• pp.97-98
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• 2010

• Journal of the Korean Magnetics Society
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• v.16 no.4
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• pp.206-210
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• 2006

A room-temperature ferromagnetism has been observed for oxygen-deficient rutile and anatase $TiO_{2-{\delta}}$ films. XPS data revealed the existence of $Ti^{3+}$ ions, for compensating the charge imbalance caused by oxygen vacancies in the film. The observed ferromagnetism is attributable to the spin ($3d^1$) alignment of the $Ti^{3+}$ ions. Such spin alignment can happen through magnetic polaron formed by trapped electron in oxygen vacancy and magnetic $Ti^{3+}$ ions around it.

• New Physics: Sae Mulli
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• v.68 no.11
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• pp.1249-1261
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• 2018

The quantitative representation for the magnetic force of a cylindrical permanent magnet acting on a ferromagnetic cylindrical object was derived on the basis of magnetization theories, and the Gilbert and Ampere models of magnetism. The magnetic force derived in this study is directly proportional to the remanent magnetization magnetic field, the cross-sectional area of the permanent magnet, the saturation magnetic field, and the cross-sectional area of the ferromagnetic object and is inversely proportional to the square of the quantity related to the distance between the permanent magnet and the ferromagnetic object. The magnetic forces of an AlNiCoV cylindrical permanent magnet and a Ferrite cylindrical permanent magnet, both with a radius of 0.4 cm and a length of 7 cm, acting on ferromagnetic objects at distances farther than the radius were calculated to be less than 3.6711 N and 0.1857 N, respectively.

• Journal of the Korean Magnetics Society
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• v.21 no.1
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• pp.10-14
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• 2011

We have measured the ferromagnetic resonance (FMR) signal in as deposited and $400^{\circ}C$ annealed CoFeB/MgO thin film to investigate the annealing effect on magnetic anisotropies and FMR linewidth (${\Delta}H_{PP}$). The uniaxial anisotropy field ($H_{K1}$) was only observed in the as deposited sample. Whereas, in the $400^{\circ}C$ annealed sample, the biaxial anisotropy field ($H_{K2}$) was additionally observed in accompany with uniaxial anisotropy field ($H_{K1}$). The appearance of biaxial anisotropy fields was originated from the crystalline growth of bcc CoFeB(001) from the MgO(001) interface and by the B diffusion during thermal annealing. Also, the ${\Delta}H_{PP}$ of $400^{\circ}C$ annealed sample was increased compared with that of as deposited sample, which was due to the broad distribution of the magnetization axis by the biaxial anisotropy.

• Journal of the Korean Magnetics Society
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• v.3 no.2
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• pp.125-129
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• 1993

The magnetic properties of RF magnetron sputtered $Co_{79}Cr_{21}(at.%)$ thin film have been examined by using of ferromagnetic resonance. The properties of $Co_{79}Cr_{21}$ thin film show the effective first order anisotropy constant of $2.91{\times}10^{5}\;erg/cm^{3}$, the effective anisotropy field of 2526 Oe, and the spectroscopic splitting factor of 2.17. The torque experimental results, analyzed by employing modified Artman method, coincide with the ferromagnetic res-onance experimental results.

• Journal of the Korean Magnetics Society
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• v.26 no.2
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• pp.50-54
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• 2016

We analyzed the angular dependence of ferromagnetic resonance linewidth in exchange coupled CoFe/MnIr bilayers. The maximum and minimum linewidth was observed in the easy and hard direction of unidirectional anisotropy by exchange coupling, respectively, and it was well agreed with the angular dependence of exchange bias field. The maximum linewidth was due to the twist of CoFe magnetization near CoFe/MnIr interface from direction of pinned MnIr spin to direction of applied magnetic field. While, minimum linewidth more higher than that of CoFe was related to rotatable anisotropy field, and explained by easy axis distribution of MnIr grains.