• Analytical Science and Technology
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• v.12 no.6
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• pp.484-489
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• 1999

The extraction of trace amounts of Se in volcanic rock was investigated using the hydride generation method and atomic absorption spectrophotometry. The powdered rock, 1.0 g, was decomposed with the mixture of $HClO_4$, $HNO_3$ and HF in an acid digestion bomb at $140^{\circ}C$ for 2 hours. For the reduction of Se(VI) to Se(IV) in the solution, 10 mL of 6 M HCl and 0.2 mL of 1 M KBr were added to the solution and the mixture was heated for 30~45 minutes. $H_2Se$ was produced by adding 3% $NaBH_4$ as a strong reducing agent, extracted by nitrogen gas, and was absorbed twice into $KMnO_4$solution. The contents of Se in the solution were determined by generation/AAS. According to the proposed method, 1.0 ng or more of Se was quantitatively extracted and Se levels of 2.5 ng/g or more in rock samples could be determined. For example, Se in a rhyolite was determined with the precision of $19.5{\pm}1.3ng/g$(95% confidence, n=6).

• Journal of Magnetics
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• v.12 no.4
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• pp.137-140
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• 2007

We have studied the temperature dependent magnetic properties and crystalline phase transitionn in small amount Fe doped nickel chromite. The Crystalline structure of $NiCr_{1.7}Fe_{0.3}O_4$ is spinel cubic (Fd-3m) structure with a lattice constant $a_0=8.317\AA$ at room temperature. The magnetic $N\acute{e}el$ temperature $(T_N)$ of the Fe doped nickel chromite sample is determined to be 250 K. The $M\ddot{o}ssbauer$ spectra exhibit that there are two magnetic phases with the two different sites for the $Cr^{3+}$ ions. The spectrum at 4.2 K is fitted to two magnetic components of the magnetic hyperfine fields $H_{hf}=496$ and 485 kOe. From the spectrum at 295 K, the electric quadrupole splittings are observed with large values of 0.49 and 0.50 mm/s, respectively. The values of the isomer shifts at all temperature ranges show that the Fe ions are ferric states. We are suggested that the dynamic Jahn-Teller distortion and anisotropic magnetic relaxation effects due to the crystalline phase transition.

• Journal of the Korean Society for Heat Treatment
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• v.20 no.6
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• pp.299-305
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• 2007

The effect of spray deposition of oxide particles on oxidation behaviors of as-cast Mo-14.2Si-9.6B (at%) alloys at $1200^{\circ}C$ up to for 100 hrs has been investigated. Various oxide powders are utilized to make coatings by spray deposition, including $SiO_2,\;TiO_2,\;ZrO_2,\;HfO_2$ and $La_2O_3$. It is demonstrated that the oxidation resistance of the cast Mo-Si-B alloy can be significantly improved by coating with those oxide particles. The growth of the oxide layer is reduced for the oxide particle coated Mo-Si-B alloy. Especially, for the alloy with $ZrO_2$ coating, the thickness of oxide layer becomes only one fifth of that of uncoated alloys when exposed to in air for 100 hrs. The reduction of oxide scale growth of the cast Mo-Si-B alloy due to oxide particle coatings are discussed in terms of the change of viscosity of glassy oxide phases that form during oxidation at high temperature.

• Journal of the Korean Physical Society
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• v.73 no.11
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• pp.1708-1711
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• 2018

The polycrystalline sample of $Ba_2Co_{1.5}Mg_{0.5}Fe_{11.88}Ga_{0.12}O_{22}$ Y-type hexaferrite, doped with Ga-cation, was prepared by using the solid-state reaction method. The crystalline structure of sample was investigated by x-ray diffractometer (XRD), and the magnetic properties of sample were measured by vibrating sample magnetometer (VSM), and $M{\ddot{o}}ssbauer$ spectrometer. The crystal structure of prepared sample was determined to be rhombohedral with space group R-3m. From the temperature dependence of the magnetization curves under 100 Oe between 4.2 and 740 K, two temperature-dependent magnetic transitions occurred in the $Ba_2Co_{1.5}Mg_{0.5}Fe_{11.88}Ga_{0.12}O_{22}$ sample. $M{\ddot{o}}ssbauer$ spectra of the sample were analyzed at various temperatures ranging from 4.2 to 620 K, and the $Ba_2Co_{1.5}Mg_{0.5}Fe_{11.88}Ga_{0.12}O_{22}$ sample showed abrupt changes in $H_{hf}$ and $E_Q$ at 200 K, indicating the spin transition effect. We have also determined the magnetic transition temperature $T_C$, in addition to the temperature dependent magnetization and ZVC measurements.

• Proceedings of the Korean Vacuum Society Conference
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• 2012.08a
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• pp.165-165
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• 2012

비정질의 Tantalum-indium-zinc oxide (TIZO) 박막 트랜지스터는 RF-sputtering 방법으로 증착되었으며 소결된 단일 타겟을 사용하였다. 증착당시 반응 가스는 알곤과 산소를 95 : 5로 섞어 반응성 스퍼터링을 진행하였으며, 1 mtorr에서 5 mtorr까지 다양한 공정압력에서 증착한 이 후 Furnace system을 통하여 $350^{\circ}C$의 온도로 1시간 동안 후열처리 공정을 진행하였다. 비정질 TIZO 박막을 활성 층으로 사용하여 제작한 박막 트랜지스터는 공정압력이 낮아짐에 따라 높은 이동도와 낮은 subthrehsold gate swing 보였다. 이러한 현상의 원인을 규명하고자 물리적, 전기적, 광학적 분석을 통하여 공정압력의 변화가 박막 트랜지스터 구동에 미치는 영향을 해석하였다. 우선 공정압력에 따른 TIZO 박막의 Ta, In, Zn, O 각각의 조성을 분석하기 위하여 Rutherford back scattering (RBS) 분석을 실시하였다. 또한 X-선 회절(X-ray diffraction)분석을 통해 열처리된 TIZO 박막은 공정압력에 따라 물리적 구조의 변화를 일으키지 않으며 모든 박막은 비정질상을 보이는 것을 확인하였다. 3.3eV의 광학적 밴드 갭은 기존에 보고되었던 비정질 산화물 반도체(InGaZnO, HfInZnO 등)와도 유사한 밴드갭을 가지고 있음을 확인하였다. 또한, spectroscopic ellipsometry (SE)분석을 통하여 전도대 이하 밴드 갭 내에 존재하는 결함상태 및 전도대에서 결함상태까지의 에너지 준위 그리고 공정압력에 따라 결함의 양과 발생되는 에너지 준위가 변화하는 현상을 관측하였다. 박막을 제조 할 때의 공정압력은 박막 내의 결함의 양 및 발생되는 에너지 준위의 변화를 야기하고 변화된 결함의 양과 발생된 에너지 준위에 따라 박막트랜지스터의 전기적 특성을 변화시킨다는 결과를 도출하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.02a
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• pp.128-128
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• 2011

Polysilicon thin-film transistors (poly-Si TFTs)는 능동행렬 액정 표시 소자(AMLCD : Active Matrix Liquid Crystal Display)와 DRAM과 같은 메모리 분야에 폭넓게 적용이 가능하기 때문에 많은 연구가 진행되고 있다. 최근 poly-Si TFTs의 우수한 특성으로 인하여 주변 driving circuits에 직접화가 가능하게 되었다. 또한 디스플레이 LCD 패널에 controller와 메모리와 같은 다 기능의 장치을 직접화 하여 비용의 절감과 소자의 소형화가 가능한 SOP (System on panels)에 연구 또한 진행 되고 있다. 이미 잘 알려진 바와 같이 비휘발성 메모리는 낮은 소비전력과 비휘발성이라는 특성 때문에 이동식 디바이스에 데이터 저장 장치로 많이 사용되고 있다. 하지만 플로팅 타입의 비휘발성 메모리는 제작공정의 문제로 인하여 SOP의 적용에 어려움을 가지고 있다. SONOS 타입의 메모리는 빠른 쓰기/지우기 효율과 긴 데이터 유지 특성을 가지고 있으나 소자의 스케일링 따른 누설전류의 증가와 10년의 데이터 보존 특성을 만족 시킬 수 가 없는 문제가 발생한다. 본 연구에서는 SOP 적용을 위하여 ELA 방법을 통하여 결정화한 poly-Si TFT memory를 SiO2/Si3N4/SiO2 Tunnel barrier와 High-k HfO2과 Al2O3을 Trapping layer와 Blocking layer로 적용, 비휘발성 메모리을 제작하여 전기적 특성을 알아보았다.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.9 no.5
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• pp.463-469
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• 1999

The potassium lithium niobate $K_3$$Li_2$$Nb_5$$O_{15}$ single crystals were growing in $K_x$$Li_{1-x}$$NbO_3$ (x = 0.4~0.6) chemical formular by the Czorchralski method. Crystal growth is studied in two orientations with growth along a-axis and c-axis. We have subjected this crystal to x-ray diffraction studies and found that they are single-crystalline and belong to tetragonal system with the lattice parameters a = b = 12.577 $\AA$ and c = 3.997$\AA$. The temperature dependence of dielectric constant was measured in the region of the phase transition. Curie temperature and diffuseness of phase transition are influenced by composition concentration. The composition and cation distribution of ferroelectric TB-type niobate crystals has a strong influence on the ferroelectric properties. Growth condition, optical transmittance, etching pattern and dielectric properties are presented and discussed.

• Journal of Life Science
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• v.21 no.9
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• pp.1214-1218
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• 2011

We investigated the fruits of Rubus crataegifolius Bge, a plant which has been traditionally used in Korea in phytotherapy, to describe antioxidant materials from plant sources. R. crataegifolius fruits were extracted with methanol and further fractionated into n-hexane, diethyl ether, and ethyl acetate. The antioxidant activity of each fraction and the residue was assessed using a 1,1-diphenyl-2-picrylhydrazyl (DPPH), $H_2O_2$ radical scavenging method, and their cytotoxicity on human primary kerationcyte (HK) was determined by an MTS assay. The R. crataegifolius fruit methanol extract showed strong antioxidant activity (75.04%, 50%) compared with vitamin C (79.9%, 54.1%) by the DPPH, and $H_2O_2$ method, respectively. The measured activity from the subsequent extracts of the methanol extract were 20.3% for n-hexane fraction (HF), 68.8% for diethyl ether fraction (DF), 67.1% for ethyl acetate fraction (EF), and 67.1% for the residue fraction (RE) by DPPH and 2.2% for HF, 1.6% for DF, 10% for EF, and 50% for the RE by $H_2O_2$ assay. An oxidative stress model of HK was established under a suitable concentration (1 mM). The cell viability of the RE treated group increased and the percentage of apoptotic cells decreased at concentrations of 0.005-0.02% RE compared with the $H_2O_2$ treated group. Fruit extracts of the medicinal plant R. crataegifolius showed potent antioxidant activity and the ability to relieve cell damage from $H_2O_2$ induced injury to HK.

• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.161.1-161.1
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• 2016

박막 태양전지의 광 산란을 위한 텍스쳐 된 표면은 반사 손실을 감소시키기 위한 것이다. 그러나, 투명한 전극(TCO)의 텍스쳐 된 표면은 빛의 가용성을 제한하고, 장파장 영역에서 haze의 수치를 감소시키며, 전반사의 증가는 박막 태양전지의 Jsc를 감소시킨다. 본 논문에서는 높은 빛의 가용성을 위하여 HF+HCl 혼합용액을 이용하여 표면의 질을 향상시키기 위한 해결책을 제시했다. 같은 HF+HCl 혼합용액을 사용하여, 540 nm의 파장에서 약 85 %의 높은 haze 수치를 달성했으며, ZnO:Al 막의 증착 후에 식각된 유리 기판과 함께 비교했을 때, 2.3%의 haze 수치의 감소를 얻었다. 또, 깊은 습식 식각에 의하여 Haze 수치를 증가시키기 위한 메커니즘 간단히 설명했다. 텍스쳐 된 유리 기판의 haze 수치의 측면에서 광학 이득은 일반적인 Asahi FTO 유리(${\lambda}=540nm$의 13.5%)에 비해 상당히 높다. 이러한 높은 haze 수치의 AZO 박막은 박막 태양전지의 Jsc를 개선하는데 이용할 수 있다.

• Transactions of the Korean hydrogen and new energy society
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• v.22 no.2
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• pp.206-212
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• 2011

The effect of process parameters on $H_2$ production from water vapor excited by HF ICP has been qualitatively examined for the first time. With the increase of ICP power, characteristics of $H_2$ production from $H_2O$ dissociation in plasma was divided into 3 regions according to both reaction mechanism and energy efficiency. At the edge of region (II) in the range of middle ICP power, energy effective hydrogen production from $H_2O$ plasma can be achieved. Furthermore, within the region (II) power condition, heating of substrate up to $500^{\circ}C$ shows additional increase of 70~80% in $H_2$ production compared to $H_2O$ plasma without substrate heating. This study have shown that combination of optimal plasma power (region II) and wall heating (around $500^{\circ}C$) is one of effective ways for $H_2$ production from $H_2O$.