최선근 교수
Seon-Keun Choi
한양대학교 물리학과 · 재료과학
연구실 소개
최선근 교수의 연구실은 나노구조 페라이트 및 페로마그네틱 나노입자를 합성하고, 그들의 자기적 특성과 응용 가능성을 탐구하는 데 중점을 두고 있습니다. 특히 자가연소법을 활용한 나노복합재료 제조와 수소 환원 공정을 통해 고자기화도를 가지는 α-Fe/산화물 코어-쉘 나노입자를 개발하며, 고주파 영역에서의 낮은 손실과 안정된 투자율을 확보한 응용 기술 개발에도 기여하고 있습니다. 또한 플라즈마 내 미세먼지 입자의 전하 및 상호작용 메커니즘을 분석함으로써, 반도체 공정 등 응용 분야에서의 플라즈마 안정성 향상에 기여하고자 합니다.
연구 현황
연구 성과 추이
표시된 성과는 수집된 데이터 기준으로 산출되며, 일부 차이가 있을 수 있습니다.
주요 논문
5Abstract Ba‐hexaferrite and Ni 0.5 Zn 0.5 ferrite nano composites have been successfully fabricated by a self‐propagating combustion method. Transmission electron microscopy and X‐ray diffractometer analysis showed that two ferrite phases were homogeneously distributed and the measured grain size of them around 20nm. The saturation magnetizations of the composites were revealed to be increased compared with the theoretical values. These increments of the saturation magnetization values could be
Ferromagnetic nanoparticles with a core/shell structure were fabricated by a self-propagating combustion method and subsequent hydrogen reduction process. Before the reduction process, synthesized particles were Fe oxide phases. Transmission electron micrographs confirmed that the nanoparticles were composed of α-Fe core and Fe–Al oxide shell after the reduction process. The saturation magnetization of the nanoparticles was measured about 180 emu/g and the permeability kept constant value of abo
Abstract A broadband coplanar waveguide method, recognized as a simple and effective broadband permeability measurement tool, was used to measure the frequency dependent permeability of various magnetic thin films. It was revealed that measured permeability was strongly dependent on the dimension of the films and the geometry of the waveguide. This dependency was proven to result from the confinement of magnetic fields in the films by LLG equation. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, W
We investigated charged dust and its effect on RF plasma by using a planar electric probe in a large-scale device. In background plasmas, the particle density is 108 to 109 cm−3 and the electron temperature is 2 to 4 eV. When dust is contained in plasma, it is negatively charged by electrons attached to the dust. The charged dust density and the charge were calculated by comparing dusty helium plasma to pure helium plasma. Depending on the increase in the amount of dust, the charged dust density
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