• 한국표면공학회지
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• 제39권5호
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• pp.206-209
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• 2006

Indium tin oxide (ITO) films were synthesized on polymer (PES, polyethersulfone) at room temperature by pulsed DC magnetron sputtering. By the control of introducing hydrogen to argon atmosphere, the resistivity of ITO films was obtained at $5.27\;{\times}\;10^{-4}\;{\Omega}{\cdot}cm$ without substrate heating in comparison with $2.65\;{\times}\;10{-3}\;{\Omega}{\cdot}cm$ under hydrogen free condition. ITO film synthesized at Ar condition was changed from amorphous to crystalline. These result from the enhancement of electron temperature in $Ar\;+\;H_2$ plasma, which induces the increase of ionization of target materials and argon. The dominant increase of ions such as In II and O II and neutral Sn I was monitored by optical emission spectroscopy (OES). Thermal energy required for the crystalline film formation is compensated by kinetic energy transfer through ion bombardments to substrate.

• 한국항해항만학회지
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• 제34권3호
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• pp.205-211
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• 2010

밸러스트수 처리를 위한 Plasma Gun의 전기적 특성과 오존 생성에 미치는 주요 운전변수들의 영향에 관해 실험실 규모 연구를 수행하였다. 방전개시전압보다 높은 전압이 인가되면 방전이 시작되고 오존이 생성되었으며 전압이 증가함에 따라 기체로 전달되는 에너지 및 오존 농도가 거의 선형적으로 증가하였다. 오존 생성 측면에서 최적의 에너지 효율성을 얻을 수 있는 전극간 거리가 존재하였으며 실험된 장치에서는 1.95 mm의 전극간 거리에서 최적 효율이 얻어졌다. 전기에너지 특성에 미치는 내부전극 재질의 영향은 무시할만한 수준이었으나 내부전극의 전기전도도와 열전도도 차이가 오존 생성에 큰 영향을 미치는 것으로 나타났다. 일정한 Plasma Gun 구조에서 오존 생성은 기체로 전달되는 에너지밀도에 의해 중요한 영향을 받는 것으로 나타났으며 유입되는 기체의 산소함량이 증가할수록 오존 생성이 증가하는 것으로 나타났다.

• Bulletin of the Korean Chemical Society
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• 제34권2호
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• pp.531-538
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• 2013

A mass balance method established in this laboratory was applied to determine the purity of an endosulfan-II pure substance. Gas chromatography-flame ionization detector (GC-FID) was used to measure organic impurities. Total of 10 structurally related organic impurities were detected by GC-FID in the material. Water content was determined to be 0.187% by Karl-Fischer (K-F) coulometry with an oven-drying method. Non-volatile residual impurities was not detected by Thermal gravimetric analysis (TGA) within the detection limit of 0.04% (0.7 ${\mu}g$ in absolute amount). Residual solvents within the substance were determined to be 0.007% in the Endosulfan-II pure substance by running GC-FID after dissolving it with two solvents. The purity of the endosulfan-II was finally assigned to be ($99.17{\pm}0.14$)%. Details of the mass balance method including interpretation and evaluating uncertainties of results from each individual methods and the finally assayed purity were also described.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2006년도 제37회 하계학술대회 논문집 C
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• pp.1629-1630
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• 2006

This paper describes a micro total analysis system ($\mu$ TAS) for detecting and digesting the target protein which includes a bead based temperature controllable microchip and computer based controllers for temperature and valve actuation. We firstly combined the temperature control function with a bead based microchip and realized the on-chip sequential reactions using two kinds of beads. The PEG-grafted bead, on which RNA aptamer was immobilized, was used for capturing and releasing the target protein. The target protein can be chosen by the type of RNA aptamer. In this paper, we used the RNA aptamer of HCV replicase. The trypsin coated bead was used for digesting the released protein prior to the matrix assisted laser desorption ionization time of flight mass spectrometer (MALDI TOF MS). Heat is applied for release of the captured protein binding on the bead, thermal denaturation and trypsin digestion. PDMS microchannel and PDMS micro pneumatic valves were also combined for the small volume liquid handling. The entire procedures for the detection and the digestion of the target protein were successfully carried out on a microchip without any other chemical treatment or off-chip handling using $20\;{\mu}l$ protein mixture within 20 min. We could acquire six matched peaks (7% sequence coverage) of HCV replicase.

• 한국광물학회지
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• 제18권1호
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• pp.53-59
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• 2005

예천지역 화강섬록암 풍화단면내의 흑운모가 산화흑운모로 풍화되는 과정에서 Rb-Sr 동위원소연대의 변화를 분석하였다. 신선한 흑운모와 풍화된 흑운모들의 Rb-Sr 동위원소 조성을 열이온화질량분석기로 측정하였고, 이를 기존의 K-Ar 자료와 비교하였다. Rb-Sr 동위원소연대는 흑운모의 산화정도에 따라 체계적으로 감소하는 경향을 보이며, 이는 K-Ar 연대의 감소경향과 잘 일치하였다. Fe/sup 2+/의 산화로 발생하는 과잉전하로 구조내 양이온들이 방출되는 과정에서 층간의 방사기원핵종도 일부 방출되었는데, 일가 양이온인 /sup 87/Rb이 이가 양이온인 /sup 87/Sr로 붕괴되어 딸핵종인 /sup 87/Sr이 모핵종인 /sup 87/Rb보다 심하게 흑운모로부터 제거된 것으로 보이고, 그 결과 Rb-Sr 동위원소연대가 감소하였다. 풍화된 흑운모는 모암의 연대측정대상으로 부적합한 것으로 보이지만, 풍화과정에서 방사기원 동위원소들의 거동은 흑운모 풍화의 지화학적 및 구조적 과정에 대한 유용한 정보를 제공한다.

• 보존과학회지
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• 제35권3호
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• pp.209-216
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• 2019

청주 송절동유적 출토 마형대구 29점의 납동위원소비 분석결과를 활용하여 납의 원료산지를 확인하고, 출토지와의 연관성을 확인하고자 하였다. 먼저 동북아시아 방연석 분포도(Mabuchi, 1985) 대입결과 대부분 중국 남부영역 내에서 매우 밀집한 분포 경향성을 나타내었으며, 한반도 납동위원소 분포도 적용결과 전라도와 충청도 지역에 해당하는 영남육괴 및 옥천변성대 지역인 Zone 3으로 확인되었다. 따라서 청주 송절동유적 출토 마형대구는 출토지와 유사한 지역에 위치한 방연석 광산에서 채취한 원료를 사용하여 제작하였을 것으로 볼 수 있다. 이와 함께 한반도 마형대구 출토 중심지역에 해당하는 중서부지역의 미호천유역 및 안성천유역 출토 마형대구 38점의 납동위원소비 분석결과와 비교하여 해당 문화권 내 마형대구 제작에 사용된 납 원료산지의 연관성 및 지역적 특성을 확인하였다. 향후 시대적 지역적 특성을 나타내는 마형대구를 대상으로 한 납동위원소비 분석결과를 축적하여 추가적인 원료산지 비교분석 연구를 통해 한반도 출토 마형대구의 납 원료산지에 대한 종합적인 정보를 얻을 수 있을 것으로 생각된다.

• 한국군사과학기술학회지
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• 제24권2호
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• pp.211-218
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• 2021

This paper deals with the computational work to characterize the formation and pinching of a plasma in an X-pinch configuration. A resistive magnetohydrodynamic model of a single fluid and two temperature is adopted assuming a hollow conical structure in the (r,z) domain. The model includes the thermodynamic parameter of tungsten from the corrected Thomas-Fermi EOS(equation of state), determining the average ionization charge, pressure, and internal energy. The transport coefficients, resistivity and thermal conductivity, are obtained by the corrected Lee & More model and a simple radiation loss rate by recombination process is considered in the simulation. The simulation demonstrated the formation of a core-corona plasma and intense compression process near the central region which agrees with the experimental observation in the X-pinch device at Seoul National University. In addition, it confirmed the increase in radiation loss rate with the density and temperature of the core plasma.

• 분석과학
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• 제18권1호
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• pp.27-34
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• 2005

보론 동위원소 표준물을 이용하여 $Li_2B_4O_7$와 $Na_2B_4O_7$를 합성하고 이로부터 $Li_2BO_2{^+}$ (질량 56, 57)와 $Na_2BO_2{^+}$ (질량 88, 89)를 열 이온화 질량분석기를 이용하여 양이온 질량분석법(PTIMS)으로 측정하였으며 또한 같은 시료를 음이온 질량분석법 (NTIMS)으로 $^{10}BO_2{^-}$와 $^{11}BO_2{^-}$ (질량 42와 43)를 보론 (질량 10, 11)대신 측정하였다. 이들 방법 간의 정밀도와 정확도를 비교하고, 각각의 방법에서 동중원소 영향이 있는지를 알아보았다. 세 가지 방법 중에 NTIMS 방법이 제일 좋은 결과를 보여주었으며 작은 시료 양으로도 안정된 피크를 얻을 수 있었다. NTIMS 방법으로 지하수 약 $5{\mu}L$(약 8 ng-B)를 직접시료로 사용하여 보론 동위원소 비를 측정하여 상대 표준편차 0.03%의 결과를 얻었다. 또한 NTIMS-IDMS로 보론을 정량한 결과 $1.65{\pm}0.003{\mu}g-B/mL$을 얻었으며 ICP-AES 결과에 비해 좋은 정밀도를 보였다.

• Journal of Radiation Protection and Research
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• 제43권3호
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• pp.120-123
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• 2018

Background: Analysis of enrichment of $UO_2$ is important to verify the information declared by the license-holders. The redundancy methods are required to guarantee the analysis result. Korea Institute of Nuclear Nonproliferation and Control (KINAC) used to analyze it with alpha spectrometry and consign to Korea Basic Science Institute (KBSI) Thermal Ionization Mass Spectrometry (TIMS). This article evaluated the similarity of the results with two methods and derive correlation equation. It could be compared to the results measured by TIMS running by KBSI. Materials and Methods: There are not many certified materials for the uranium enrichment value. Therefore, 34 uranium pellets, which have the wide range of uranium enrichment from 0.21 to 4.69 wt%, were used for the experiments by the alpha spectrometry and the TIMS. Results and Discussion: The study shows there are the tendency of analyzed enrichment by each equipment. It shows uranium enrichment with alpha spectrometry evaluated 17% higher than that with TIMS on average. The regression equations were also derived in case the similarity between the two results with two methods is lower than predicted. Two experiments were designed to compare the effect of number of samples. The $R^2$ was 0.9977 with 34 pellets. It shows the equation is appropriate to predict the enrichment values by TIMS with that of alpha spectrometry. The $R^2$ was 0.9858 with four pellets for ten times. The $R^2$ decreased while the number of samples increased. The discrepancy between the lowest and highest enrichment seems to be one of the reason for it. Conclusion: KINAC expects the first equation with 34 samples is useful to predict the result with TIMS, the redundancy method, based on the alpha spectrometry. The extra samples are necessary to collect if the enrichment value analyzed by TIMS is lower than the value predicted with the equation. Further study would be followed related to the impact of the peak counts for each uranium isotopes, sample amount and number of experiments when TIMS established in KINAC by the end of 2018.

• 한국안전학회지
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• 제32권2호
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• pp.34-37
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• 2017

In recent emerging industry, Display field becomes bigger and bigger, and also semiconductor technology becomes high density integration. In Flat Panel Display, there is an issue that electrostatic phenomenon results in fine dust adsorption as electrostatic capacity increases due to bigger size. Destruction of high integrated circuit and pattern deterioration occur in semiconductor and this causes the problem of weakening of thermal resistance. In order to solve this sort of electrostatic failure in this process, Soft X-ray ionizer is mainly used. Soft X-ray Ionizer does not only generate electrical noise and minute particle but also is efficient to remove electrostatic as it has a wide range of ionization. X-ray Generating efficiency has an effect on soft X-ray Ionizer affects neutralizing performance. There exist variable factors such as type of anode, thickness, tube voltage etc., and it takes a lot of time and financial resource to find optimal performance by manufacturing with actual X-ray tube source. MCNPX (Monte Carlo N-Particle Extended) is used for simulation to solve this kind of problem, and optimum efficiency of X-ray generation is anticipated. In this study, X-ray generation efficiency was measured according to target material thickness using MCNPX under the conditions that tube voltage is 5 keV, 10 keV, 15 keV and the target Material is Tungsten(W), Gold(Au), Silver(Ag). At the result, Gold(Au) shows optimum efficiency. In Tube voltage 5 keV, optimal target thickness is $0.05{\mu}m$ and Largest energy of Light flux appears $2.22{\times}10^8$ x-ray flux. In Tube voltage 10 keV, optimal target Thickness is $0.18{\mu}m$ and Largest energy of Light flux appears $1.97{\times}10^9$ x-ray flux. In Tube voltage 15 keV, optimal target Thickness is $0.29{\mu}m$ and Largest energy of Light flux appears $4.59{\times}10^9$ x-ray flux.