• Title/Summary/Keyword: 벌크 재료

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Surface Micromachining for the Micro-heater Fabrication of Gas Sensors (가스 센서용 마이크로 히터의 표면 마이크로머시닝 기술)

  • Lee, Seok-Tae;Yun, Eui-Jung;Jung, Il-Yong;Lee, Kang-Won;Park, Hyung-Sik
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2006.06a
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    • pp.352-353
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    • 2006
  • 가스센서용 마이크로 히터 제작에는 표연 마이크로 머시닝 또는 벌크 마이크로머시닝 기술을 이용한다. 표면 마이크로 머시닝에 의한 마이크로 히터 (MHP) 구조의 경우, 기판과 박막간의 폭이 좁기 때문에 에칭 공정 후 세정이 잘 이루어지지 않으면 열적 절연이 잘 이루어지지 않아서 히터와 센서의 성능을 저하시키는 원인이 된다. 본 연구에서는 표면 마이크로 머시닝 기술에 의한 가스 센서용 마이크로 히터를 제작한다. $SiO_2$$Si_3N_4$를 성분으로 하며, $100{\mu}m\;{\times}\;100{\mu}m$의 면적과 350 nm 의 두께를 갖는 가스 센서용 마이크로 히터를 제작하였다. 이를 위하여 ANSYS를 통한 유한요소해석에 의한 열분포 해석으로 최적구조를 확인하였다. 센서로의 열 전달 효율을 높이기 위해 센서 박막은 히터 위에 적층하였다. 실리콘 표면과 마이크로 히터와의 간격은 에칭 공정을 통하여 $2{\mu}m$로 하였으며, 이 공간에서는 에칭 및 세정 후에 이물질이 깨끗이 세정되지 않고 남아 있거나, 습식 공정 중에 수분의 장력에 의한 열전연성이 나빠질 수 있는 등 단점이 있다. 이는 건식 등방성 에칭 공정을 통하여 해결하였다.

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Characteristics of impedance spectroscopy depending on thickness of emissive layer in Organic Light-Emitting Diodes (유기발광소자의 발광층 두께변화에 따른 임피던스 특성 분석)

  • Ahn, Joon-Ho;Lee, Joon-Ung;Chung, Dong-Hoe;Lee, Sung-Ill;Song, Min-Jong;Kim, Tae-Wan
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2005.05a
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    • pp.193-196
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    • 2005
  • 유기발광소자의 발광층의 두께에 따른 임피던스의 변화를 살펴보았다. 임피던스는 두께에 따라 저항의 변화에 따른 의존성을 보이며, 그에 따른 임피던스와 Cole-Cole 반원의 변화, 두께에 따른 $1/\tau$ 의 변화를 살펴보았다. 발광층의 두께는 각각 100, 200, 300 nm의 두께로 열증착하여 실험하였고, 소자의 구조는 $ITO/Alq_3/Al$의 구조로 측정 하였다. 유기발광소자의 발광층인 $Alq_3$의 두께가 증가함에 따라 임피던스의 크기가 증가하고, 위상각의 크기는 100nm의 경우 0V에서 용량성을 보이다가 6~10V까지 부성저항특성을 나타낸 후 약 22V에서 저항성을 나타내고, 200과 300 nm의 경우 12V까지 용량성을 나타내다 이후 22V 근방에서 $0^{\circ}$에 가까워지며 저항성을 나타내는 것을 알 수 있었다. 또한 두께에 따른 Cole-Cole 반원을 살펴보면 두께가 증가할수록 반원의 크기가 증가하는 것을 알 수 있으며, 이를 통해 간단한 등가회로를 예측할 수 있었다. 그리고 벌크내의 용량성$(C_p)$을 측정하여 두께의 증가에 따라 $C_p$ 값이 감소하는 것을 알 수 있었다.

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The study for phase change properties of Se added $Ge_2Sb_2Te_5$ thin films ($Ge_2Sb_2Te_5$ 박막의 Se 증가에 따른 상변화 특성 연구)

  • Lim, Woo-Sik;Kim, Sung-Won;Lee, Hyun-Yong
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.06a
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    • pp.166-166
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    • 2007
  • PRAM (phase-change random access memory)은 전류 펄스 인가에 따른 기록매질의 비정질-결정질 간 상변화와 그에 동반되는 저항변화를 이용하는 차세대 비휘발성 메모리 소자로서 연구되어지고 있다. 본 논문에서는 $(Ge_2Sb_2Te_5)_{1-x}Se_x$ (x=0,0.05,0.1,0.15) 조성에 대한 벌크 및 박막시료를 제작하고 각 조성에 대한 상변화 특성을 분석하였다. XRD를 통해 열처리 온도에 따른 구조적 분석을 실시하였고 UV-Vis-IR spectrophotometer를 사용하여 박막의 광학적 특성을 분석하였다. 또한 각 조성의 결정화 속도를 비교하기 위해 static tester를 사용하여 레이저 펄스 시간에 대한 반사도 변화를 측정하였고 DSC를 통해 결정화 온도를 측정하였다.

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Neutron Irradiation Effect of YBa2Cu3O7-y Superconductor (YBa2Cu3O7-y 초전도 벌크의 중성자 조사 효과)

  • Lee, Sang Heon
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.34 no.6
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    • pp.438-441
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    • 2021
  • The electrical characteristics of single-crystal composite superconductors produced by a melting process were studied by neutron irradiation. In order to improve the current characteristics of the YBa2Cu3O7-y superconductor, it is necessary to form an effective flux pinning center inside the superconductor. In this study, an increase in flux pinning was attempted through neutron irradiation onto YBa2Cu3O7-y superconductors. The neutron irradiation was performed at 30 MeV for 500 sec, The electrical properties of the superconductors were measured in a magnetic field of 5 Tesla at 50 K using a magnetic properties measurement system (MPMS). After neutron irradiation, the critical current density of the YBa2Cu3O7-y superconductor in a 1 Tesla magnetic field was 1×105 A/cm2. Once neutrons were irradiated at 30 MeV and 10 μA for 500 sec, the critical current density was observed to increase significantly. When neutrons are irradiated to a superconductor, micro-defects are created in the superconductor, and they act as flux pinning centers that hold the magnetic field generated when an electric current flows.

Mechanical Properties of Bulk Graphite using Artificial Graphite Scrap as a Function of Particle Size (입자 크기별 가공부산물로 제조된 벌크흑연의 기계적 성질)

  • Lee, Sang Hye;Lee, Sang Min;Jang, Won Pyo;Roh, Jae Seung
    • Journal of Powder Materials
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    • v.28 no.1
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    • pp.13-19
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    • 2021
  • Bulk graphite is manufactured using graphite scrap as the filler and phenolic resin as the binder. Graphite scrap, which is the by-product of processing the final graphite product, is pulverized and sieved by particle size. The relationship between the density and porosity is analyzed by measuring the mechanical properties of bulk graphite. The filler materials are sieved into mean particle sizes of 10.62, 23.38, 54.09, 84.29, and 126.64 ㎛. The bulk graphite density using the filler powder with a particle size of 54.09 ㎛ is 1.38 g/㎤, which is the highest value in this study. The compressive strength tends to increase as the bulk graphite density increases. The highest compressive strength of 43.14 MPa is achieved with the 54.09 ㎛ powder. The highest flexural strength of 23.08 MPa is achieved using the 10.62 ㎛ powder, having the smallest average particle size. The compressive strength is affected by the density of bulk graphite, and the flexural strength is affected by the filler particle size of bulk graphite.

Changes in Flexural Strength and Electrical Resistivity of Bulk Graphite According to the Viscosity of Impregnant (함침재의 점도에 따른 벌크흑연의 굽힘강도 및 전기비저항 변화)

  • Lee, Sang-Min;Lee, Sang-Hye;Roh, Jae-Seung
    • Korean Journal of Materials Research
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    • v.31 no.2
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    • pp.108-114
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    • 2021
  • In the manufacturing of bulk graphite, pores produced by vaporization and discharge of volatile materials in binders during carbonization reduce the density of bulk graphite, which adversely affects the electrical conductivity, strength and mechanical properties. Therefore, an impregnation process is introduced to fill the pores and increase the density of bulk graphite. In this study, bulk graphite is prepared by varying the viscosity of the impregnant. The microstructure of bulk graphite is observed. The flexural strength and electrical resistivity are measured. As the viscosity of the impregnants decreases and the number of impregnations increases, it is shown that the number of pores decreases. The density before impregnation is 1.62 g/㎤. The density increases to 1.67 g/㎤ and porosity decreases by 18.6 % after three impregnations using 5.1 cP impregnant, resulting in the best pore-filling effect. After three times of impregnation with a viscosity of 5.1 cP, the flexural strength increases by 55.2 % and the electrical resistivity decreases by 86.76 %. This shows that a slight increase in density due to the pore-filling effect improves the properties of bulk graphite.

Synthesis of Al-Ni-Co-Y Bulk Metallic Glass fabricated by Spark Plasma Sintering (방전 플라즈마 소결법을 이용한 Al-Ni-Co-Y 벌크 비정질 합금의 제조)

  • Jeong Pyo Lee;Jin Kyu Lee
    • Journal of Powder Materials
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    • v.30 no.1
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    • pp.41-46
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    • 2023
  • In this study, an Al82Ni7Co3Y8 (at%) bulk metallic glass is fabricated using gas-atomized Al82Ni7Co3Y8 metallic glass powder and subsequent spark plasma sintering (SPS). The effect of powder size on the consolidation of bulk metallic glass is considered by dividing it into 5 ㎛ or less and 20-45 ㎛. The sintered Al82Ni7Co3Y8 bulk metallic glasses exhibit crystallization behavior and crystallization enthalpy similar to those of the Al82Ni7Co3Y8 powder with 5 ㎛ or less and it is confirmed that no crystallization occurred during the sintering process. From these results, we conclude that the Z-position-controlled spark plasma sintering process, using superplastic deformation by viscous flow in the supercooled liquid-phase region of amorphous powder, is an effective process for manufacturing bulk metallic glass.

Magnetic Force Properties of Superconducting Bulk (초전도 벌크의 자기적 특성을 위한 간편한 시스템)

  • Sang Heon Lee
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.36 no.1
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    • pp.70-73
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    • 2023
  • To improve superconductor properties, the size of the crystal grains of the superconductor should be adjusted, the amount of electricity flowing through the superconductor should be increased, and the superconductor should be designed to withstand external magnetic fields. It is necessary to control the microstructure so that many flux pinning centers are developed inside the superconductor so that defects are generated physically or chemically, and the micro secondary phase for trapped magnetic flux must be dispersed inside the superconductor. In order to measure the superconducting magnetic force of the superconducting bulk in a simplified manner, the superconducting magnetic force was analyzed using an Nd-Fe-B permanent magnet of 3.80 kG. In particular, by delaying the growth of partially melted Y2BaCuO5 particles, we devised a plan to refine Y2BaCuO5 particles to effectively improve superconducting magnetic force, and analyzed superconducting magnetic force in a single crystal YBa2Cu3O7-y superconducting bulk using a gauss meter. The melted superconducting bulk traps 80% or more of the applied magnetic field, and can be used as a bulk magnet of high magnetic field magnetization applicable to electric power equipment.

Artificial Neural Network Supported Prediction of Magnetic Properties of Bulk Metallic Glasses (인공신경망을 이용한 벌크 비정질 합금 소재의 포화자속밀도 예측 성능평가)

  • Chunghee Nam
    • Korean Journal of Materials Research
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    • v.33 no.7
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    • pp.273-278
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    • 2023
  • In this study, based on the saturation magnetic flux density experimental values (Bs) of 622 Fe-based bulk metallic glasses (BMGs), regression models were applied to predict Bs using artificial neural networks (ANN), and prediction performance was evaluated. Model performance evaluation was investigated by using the F1 score together with the coefficient of determination (R2 score), which is mainly used in regression models. The coefficient of determination can be used as a performance indicator, since it shows the predicted results of the saturation magnetic flux density of full material datasets in a balanced way. However, the BMG alloy contains iron and requires a high saturation magnetic flux density to have excellent applicability as a soft magnetic material, and in this study F1 score was used as a performance indicator to better predict Bs above the threshold value of Bs (1.4 T). After obtaining two ANN models optimized for the R2 and F1 score conditions, respectively, their prediction performance was compared for the test data. As a case study to evaluate the prediction performance, new Fe-based BMG datasets that were not included in the training and test datasets were predicted using the two ANN models. The results showed that the model with an excellent F1 score achieved a more accurate prediction for a material with a high saturation magnetic flux density.

Study on Surface Damage of Specimen for Transmission Electron Microscopy(TEM) Using Focused Ion Beam(FIB) (집속 이온빔을 이용한 투과 전자 현미경 시편의 표면 영향에 관한 연구)

  • Kim, Dong-Sik
    • 전자공학회논문지 IE
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    • v.47 no.2
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    • pp.8-12
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    • 2010
  • TEM is a powerful tool for semiconductor material analyses in structure or biological sample in micro structure. TEM observation need to make to coincide specimens for special purpose. in this paper, we have experimented for minimum surface damage on bulk wafer and patterned specimen by various conditions such as accelerating energy, depth of ion beam, ion milling types, and etc. in various specimen preparation methods by FIB (Focus Ion Beam). The optimal qualified specimens are contain low mounts of surface damage(about 5 nm) on patterned specimen.