• 천문학회보
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• 제41권2호
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• pp.42.1-42.1
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• 2016

The formation process and the dynamical properties of a large-scale quasi-circular flare ribbon were investigated using the SDO AIA and HMI data along with data from RHESSI and SOT. Within one hour time interval, two subsequent M-class flares were detected from the NOAA 12371 that had a ${\beta}{\gamma}{\delta}$ configuration with one bipolar sunspot group in the east and one unipolar spot in the west embedded in a decayed magnetic field. Earlier M2.0 flare was associated with a coronal loop eruption, and a two-ribbon structure formed within the bipolar sunspot group. On the other hand, the later M2.6 flare was associated with a halo CME, and a quasi-circular ribbon developed encircling the full active region. The observed quasi-circular ribbon was strikingly large in size spanning 650" in north-south and 500" in east-west direction. It showed the well-known sequential brightening in the clockwise direction during the decay phase of the M2.6 flare at the estimated speed of 160.7 km s-1. The quasi-circular ribbon also showed the radial expansion, especially in the southern part. Interestingly, at the time of the later M2.6 flare, the third flare ribbon parallel to the early two-ribbon structure also developed near the unipolar sunspot, then showed a typical separation in pair with the eastern most ribbon of the early two ribbons. The potential field reconstruction based on the PFSS model showed a fan shaped magnetic configuration including fan-like field lines stemming from the unipolar spot and fanning out toward the background decayed field. This large-scale fan-like field overarched full active region, and the footpoints of fan-like field lines were co-spatial with the observed quasi-circular ribbon. From the NLFF magnetic field reconstruction, we confirmed the existence of a twisted flux rope structure in the bipolar spot group before the first M2.0 flare. Hard X-ray emission signatures were detected at the site of twisted flux rope during the pre-flare phase of the M2.0 flare. Based on the analysis of both two-ribbon structure and quasi-circular ribbon, we suggest that a tether-cutting reconnection between sheared arcade overarching the twisted flux rope embedded in a fan-like magnetic field may have triggered the first M2.0 flare, then secondary M2.6 flare was introduced by the fan-spine reconnection because of the interaction between the expanding field and the nearby quasi-null and formed the observed large-scale quasi-circular flare ribbon.

• 청정기술
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• 제28권3호
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• pp.218-226
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• 2022

최근 선진국들은 수소경제 및 탄소중립 사회로의 전환을 위해 수소에너지의 수요가 급격히 증가하고 있으며, 이산화탄소(CO₂)를 배출이 없는 친환경적인 수소(H₂) 생산 기술에 대한 관심이 높아지고 있다. 본 연구에서는 암모니아(NH₃) 분해 수소 제조를 위해 루테늄 알루미나(Ru/Al₂O₃) 분말 촉매와 함께 알루미나 졸(alumina sol)의 무기바인더(inorganic binder)와 메틸 셀룰로오스(methyl cellulose)의 유기바인더(organic binder)를 사용하여 딥 코팅(dip coating) 방법으로 루테늄 알루미나 메탈 모노리스 코팅 촉매를 제조하였다. 딥 코팅을 위한 촉매 슬러리의 최적 비율로 촉매와 무기바인더의 중량 비율을 1:1로 고정하여 유기바인더 0.1일 때 1회 딥 코팅 시 촉매 코팅양은 61.6 g L^-1이다. 이때 메탈모노리스 표면에 코팅된 촉매 층의 균일한 두께 (약 42 ㎛)와 결정상을 주사전자현미경(Scanning Electron Microscope, SEM)과 X-ray 회절분석(X ray diffraction, XRD)을 통해 확인하였다. 또한, 암모니아 분해 수소 제조의 최적 공정조건을 찾고자 반응표면분석법(Response Surface Method, RSM)을 이용하여 반응온도와 공간속도의 독립변수에 따른 암모니아 전환율에 대한 수치 최적화 회귀식 모델을 계산하였다. 이러한 결과로부터 암모니아 분해 수소생산을 위한 상업적 규모의 공정운전 기본설계 자료로 활용이 가능하다.

• 센서학회지
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• 제12권1호
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• pp.16-23
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• 2003

Czochralski 법으로 조직등가 물질인 $Li_2B_4O_7$ 단결정을 성장하고 열형광 특성을 조사하였다. 단결정 성장시 증자결정의 회전속도는 10 rpm, 인상속도는 $0.18\;mm{\codt}h^{-1}$ 이하에서 core가 없는 양질의 단결정을 얻을 수 있었으며, X-선 회절분석을 통해 성장한 $Li_2B_4O_7$ 단결정의 구조는 정방정계임을 확인하였다. 열형광 glow 곡선은 쉽게 분해할 수 있는 세 개의 peak들이 중첩되어 나타났으며, X-선에 대한 $Li_2B_4O_7$ 단결정 TLD의 열형광감도는 50 mGy에서 1.5 Gy까지의 선량범위에서 선형적으로 나타났다. 가온율법에 의한 열형광 glow 곡선 분석과 PL 스펙트럼 분석 결과에 의한 glow peak의 활성화에너지는 각각 0.93, 1.78, 2.25 eV으로 평가되었다.

• 한국자기학회지
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• 제18권1호
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• pp.24-27
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• 2008

Polyol법을 이용하여 $MnFe_2O_4$ 나노입자를 제조하고, X-선 회절기(XRD)와 진동시료형 자화율 측정기(VSM)를 이용하여 결정학적 및 거시적인 자기적 특성을 분석하였고, 뫼스바우어($M\"{o}ssbauer$) 분광실험을 통하여 $MnFe_2O_4$ 물질의 초미세 상호작용에 대한 연구를 수행하였다. 고분해능 투과형 전자 현미경(High Resolution Transmission Electron Microscope; HRTEM)을 이용하여 입자의 크기를 분석한 결과, 대부분의 입자크기가 $6{\sim}8$ nm 정도의 분포를 가지는 매우 균일한 입자로 형성되었음을 확인할 수 있었다. X-선 회절실험의 분석 결과, $a_0=8.418{\pm}0.001{\AA}$의 격자상수를 가지는 입방정형의 스피넬 구조로써 그 공간군이 Fd3m 임을 확인하였다. 상온에서의 VSM 측정결과 강한 초상자성 거동을 보였고, 뫼스바우어 분석결과로 상온에서 초상자성 영향에 따른 요동현상이 나타남을 관측할 수 있었다. 4.2K에서는 6개의 공명흡수선이 2 set으로 존재하고 초미세 자기장 값($H_{hf}$)이 A-site의 경우 498 kOe, B-site의 경우 521 kOe 로 분석되었다.

• 한국자기학회지
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• 제8권6호
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• pp.335-340
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• 1998

거대 자기 저항 La0.67Ca0.33Mn0.9957Fe0.01O3물질을 졸-겔법을 이용하여 제조하였다. La0.67Ca0.33Mn0.9957Fe0.01O3의 자기적 성질을 X-선 회절 분석, 리더퍼스 분광 측정, 자화 측정, Mossbauer 분광 측정으로 연구하였다. 단일상 La0.67Ca0.33Mn0.9957Fe0.01O3의 결정구조는 cubic 페롭스카이트 구조이고, 격자상수 a0=3.868$\AA$이었다. 1%철 이온의 치환에 의한 격자상수의 변화는 관측할 수 없겠지만, 큐리온도는 282K에서 270K로, 77K에서의 포화 자화는 84emu/g에서 81emu/g으로 감소함을 알 수 있었다. Mossbauer 분광 측정은 4.2K에서 상온 온도 영역까지 여러 온도 구간에서 측정하였다. Mossbauer 스펙트럼의 분석은 57Fe 이온에 분포에 의한 상호작용 모델을 고려하여 분석하였다. 이성질체 이동값에 의해 철 이온은 모든 구간에서 +3가 이었다. La0.67Ca0.33Mn0.9957Fe0.01O3의 반도체-금속 전이온도는 250K이엇으며, 자기 저항비는 33%이었다..

• 한국자기학회지
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• 제15권5호
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• pp.282-286
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• 2005

공침법으로 제조한 Ni-Cu-Zn ferrite를 사용하여 전파흡수체로 사용할 저온소결용 ferrite를 연구하였다. Ni 첨가량에 따른 조성비 및 가소온도와 소결온도 변화를 시켜 전파흡수특성 및 물리적 특성을 고찰하였다. XRD pattern을 통하여 spinel구조를 가짐을 확인하였고, 공침법으로 제조된 Ni-Cu-Zn ferrite 미분말이 나노입자 크기를 보였다 소결온도가 $1100^{\circ}C$이고 Ni 함량이 많을 수록 투자율이 낮고 손실계수도 높게 측정되어 흡수 능력도 좋아짐을 알 수 있고, MHz 영역에서 사용할 수 있다고 사료된다. 그리고 소결온도 $1100^{\circ}C$이고 $(Ni_{0.7}Cu_{0.2}Zn_{0.1}O)_{1.02}(Fe_{2}O_3)_{0.98}$ 조성일 때가 가장 손실이 크므로 전파흡수체로 사용할 조성임을 확인 할 수 있었다.

• 대한한의학회지
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• 제25권4호
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• pp.43-50
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• 2004

Objective : Obesity is associated with degenerative arthropathy giving stress on joints. It also amplifies loads of weight bearing joints by changing the gravity line of the body. Our aim is to investigate the correlation between obesity and lumbar lordosis in obese pre-menopausal Korean females. The hypothesis was tested that there is a correlation between obesity and lumbar lordosis. Methods : A cross-sectional evaluation of 44 Females (baseline age 30.77 ± 6.46) with BMI 31.53 ± 3.82 (kg/㎡) was done. Body composition was measured using bio-impedance analysis (BIA), and anthropometry was done by the same observer. A lateral whole spine X-ray was taken in standing position to measure the lumbar lordotic angle (LLA), Ferguson angle (FA) and lumbar gravity line (LGL). A Pearson correlation was used to measure the correlation between obesity and lumbar lordosis (SPSS 10.0 for windows). Results : Body mass index (BMI kg/㎡) had a negative relationship with LLA((equation omitted)=-0.469), FA((equation omitted) =-0.347) and LGL((equation omitted)=-0.389). Body fat rate had a negative relationship with LLA only(γ=-0.385). Waist circumference had a negative relationship with LLA((equation omitted)=-0.345) and LGL((equation omitted)=-0.346). WH ratio had no relationship with lumbar lordosis. Conclusion : These data show that obesity is related to mechanical structures, such as lumbar lordosis. BMI was the most useful index, which reflects a change of mechanical structure of lumbar, more than other variables in this study.

• Bulletin of the Korean Chemical Society
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• 제33권5호
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• pp.1675-1680
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• 2012

Three new cyanide-bridged $Cr^{III}Mn^{II}$ binuclear complexes, $[Mn(phen)_2Cl][Cr(bpmb)(CN)_2]{\cdot}H_2O$ ($\mathbf{1}$) (phen = 1,10-phenanthroline, $bpdmb^{2-}$ = 1,2-bis(pyridine-2-carboxamido)-4-methyl-benzenate), $[Mn(phen)_2Cl][Cr(bpmb)-(CN)_2]{\cdot}H_2O$ ($\mathbf{2}$) ($bpdmb^{2-}$ = 1,2-bis(pyridine-2-carboxamido)-4,5-dimethyl-benzenate), and $[Mn(phen)_2Cl]-[Cr(bpClb)(CN)_2]{\cdot}CH_3OH{\cdot}H_2O$ ($\mathbf{3}$) ($bpClb^{2-}$ = 1,2-bis(pyridine-2-carboxamido)-4-chloro-benzenate) were obtained based on $Mn(phen)_2Cl_2$ and a series of dicyanidechromate(III) building blocks. Single crystal X-ray diffraction analysis shows the structures of the three complexes are dimeric type with two different metal centers linked by a cyanide group from corresponding dicyanidechromate(III) building block. Magnetic investigations indicate the existence of relatively weak antiferromagnetic coupling between Cr(III) and Mn(II) ions with best-fit constants $J_{CrMn}=-2.78(5)cm^{-1}$ for $\mathbf{1}$, $J_{CrMn}=-3.02(2)cm^{-1}$ for $\mathbf{2}$ and $J_{CrMn}=-2.27(3)cm^{-1}$ for $\mathbf{3}$ based on the spin exchange Hamiltonian = $-2J_{CrMn}\hat{S}_{Cr}\hat{S}_{Mn}$. The magneto-structural correlation of cyanide-bridged $Cr^{III}Mn^{II}$ complexes has been discussed at last.

• 한국재료학회지
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• 제22권2호
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• pp.78-81
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• 2012

$Y_2O_3$ nanomaterials have been widely used in transparent ceramics and luminescent devices. Recently, many studies have focused on controlling the size and morphology of $Y_2O_3$ in order to obtain better material performance. $Y_2O_3$ powders were prepared under a modified solvothermal condition involving precipitation from metal nitrates with aqueous ammonium hydroxide. The powders were obtained at temperatures at $250^{\circ}C$ after a 6h process. The properties of the $Y_2O_3$ powders were studied as a function of the solvent ratio. The synthesis of $Y_2O_3$ crystalline particles is possible under a modified solvothermal condition in a water/ethylene glycol solution. Solvothermal processing condition parameters including the pH, reaction temperature and solvent ratio, have significant effects on the formation, phase component, morphology and particle size of yttria powders. Ethylene glycol is a versatile, widely used, inexpensive, and safe capping organic molecule for uniform nanoparticles besides as a solvent. The characterization of the synthesized Y2O3 powders were studied by XRD, SEM (FE-SEM) and TG/DSC. An X-ray diffraction analysis of the synthesized powders indicated the formation of the $Y_2O_3$ cubic structure upon calcination. The average crystalline sizes and distribution of the synthesized $Y_2O_3$ powders was less than 2 um and broad, respectively. The synthesized particles were spherical and hexagonal in shape. The morphology of the synthesized powders changed with the water and ethylene glycol ratio. The average size and shape of the synthesized particles could be controlled by adjusting the solvent ratio.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 추계학술대회 논문집
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• pp.67-67
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• 2009

Due to the scaling down of the dielectrics thickness, the leakage currents arising from electron tunneling through the dielectrics has become the major technical barrier. Thus, much works has focused on the development of high k dielectrics in both cases of memories and CMOS fields. Among the high-k materials, $Al_2O_3$ considered as good candidate has been attracting much attentions, which own some good properties as high dielectric constant k value (~9), a high bandgap (~2eV) and elevated crystallization temperature, etc. Due to the easy control of ion energy and flux, low ownership and simple structure of the inductively coupled plasma (ICP), we chose it for high-density plasma in our study. And the $BCl_3$ was included in the gas due to the effective extraction of oxygen in the form of BClxOy compound. In this study, the etch characteristic of ALD deposited $Al_2O_3$ thin film was investigated in $BCl_3/N_2$ plasma. The experiment were performed by comparing etch rates and selectivity of $Al_2O_3$ over $SiO_2$ as functions of the input plasma parameters such as gas mixing ratio, DC-bias voltage and RF power and process pressure. The maximum etch rate was obtained under 15 mTorr process perssure, 700 W RF power, $BCl_3$(6 sccm)/$N_2$(14 sccm) plasma, and the highest etch selectivity was 1.9. We used the x-ray photoelectron spectroscopy (XPS) to investigate the chemical reactions on the etched surface. The Auger electron spectroscopy (AES) was used for elemental analysis of etched surface.