• 광물과 암석
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• 제35권2호
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• pp.111-123
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• 2022

본 연구는 자연계에서 가장 흔하게 관찰되는 두 그린 러스트(green rust) 광물인 carbonate green rust (CGR)과 sulfate green rust (SGR)을 공침법(co-precipitation)을 통해 각각 합성하고, 이들의 형성 메커니즘 및 이화학적 특성들을 체계적으로 규명하였다. X-선 회절(XRD) 분석 및 리트벨트 정련 수행 결과, 본 합성 조건에서 이차광물상 없이 이중층수산화물로서 CGR과 SGR이 합성됨을 확인하였다. 또한, 각각의 구조 파라미터는 CGR의 경우 a(=b)축 = 3.17 Å, c축 = 22.52 Å이고, SGR의 경우 a(=b)축 = 5.50 Å, c축 = 10.97 Å이며, 이들의 미결정 크기는 각각 (003)면 기준 57.8 nm와 (001)면 기준 40.1 nm로 밝혀졌다. 주사전자현미경/에너지 분산형 분광분석(SEM/EDS) 결과, CGR과 SGR은 모두 육각 판상의 전형적인 이중층수산화물 결정 형상을 보이지만 탄소(C)와 황(S)의 함량은 서로 다르게 나타났다. 퓨리에 변환 적외선(FT-IR) 분광 분석결과, 탄산염(CO₃^2-)와 황산염(SO₄^2-) 이온들이 각각 CGR과 SGR의 층간 음이온으로 밝혀졌고, 이는 XRD를 활용한 광물상 동정 결과와 잘 일치한다. 철 용액으로의 수산화이온(OH^-) 주입 시간에 따른 혼합 용액의 pH와 Eh, 그리고 잔류 철 농도의 비율(Fe(II):Fe(III)) 측정 결과, 시간에 따른 차이는 있지만 두 green rusts 모두 1단계 전구체 형성, 2단계 중간 생성물로의 상변환, 그리고 3단계 green rust로의 상변환과 에이징에 의한 결정성장으로 이어지는 결정 형성 메커니즘을 보이는 것으로 판단된다. 본 연구는 공침법을 통해 CGR과 SGR을 안정적으로 합성하고 이들의 형성 메커니즘과 이화학적 특성을 규명함으로써, green rust를 활용한 응용 연구 및 산업 활용에 원천 기초자료를 제공할 것으로 기대된다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2013년도 제45회 하계 정기학술대회 초록집
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• pp.228.2-228.2
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• 2013

본 논문은 InN와 GaN를 교대로 증착하는 교번성장법(Alternate Growth Method)을 이용해 형성한 높은 인듐(Indium) 조성을 갖는 InGaN (HI-InGaN) 구조의 열처리(Rapid Thermal Annealing, RTA) 온도 및 시간에 대한 구조와 광학적 특성을 Double Crystal X-ray Diffraction (DCXRD), Transmission Electron Microscopy와 Photoluminescence (PL) 장비를 사용하여 분석한 결과를 보고한다. DCXRD 스펙트럼에서 HI-InGaN 박막은 GaN(0002)로부터 $2.98^{\circ}$ 분리된 위치에서 회절 신호를 관찰 할 수 있다. 그리고 GaN와 HI-InGaN 신호 사이의 넓은 범위에서 미약하지만 신호가 관찰 되는데, 이는 InN와 GaN 계면에서 발생하는 상호확산 확률의 차이에 기인한 In 조성이 다른 InGaN 신호로 해석할 수 있다. 열처리 온도를 $775^{\circ}C$로 고정하고 시간을 10, 20, 30초로 각각 변화시켜 RTA를 진행한 DCXRD 스펙트럼에서 GaN(0002)로부터 $0.7{\sim}1.1^{\circ}$ 떨어진 위치에서 InGaN 피크를 확인 할 수 있다. RTA 시간이 증가 할수록 HI-InGaN 신호의 위치가 GaN 피크 방향으로 이동하며, 세기가 증가하는 것을 확인 할 수 있다. HI-InGaN의 PL 스펙트럼에서 상온 발광파장은 1369 nm 이며, 반치폭(Line-width)은 51.02 nm을 보였다. RTA 수행 후 발광파장에 따른 광세기가 각각 달라졌으며, 특히 900 nm 부근의 신호가 상대적으로 크게 증가하는 것을 확인할 수 있었다. RTA에 따른 HI-InGaN의 구조 및 광학적 특성 변화를 InN와 GaN 계면에서 In, Ga 원자의 상호확산 효과현상으로 논의할 예정이다.

• 대한수의학회지
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• 제32권4호
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• pp.511-521
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• 1992

The distribution of the hepatic arteries within the liver in 30 Korean native cattle were observed. Vinylite solution was injected into the hepatic arteries of 10 livers for cast preparation. The angiography was prepared in 20 livers by injected 30% barium sulfate solution into the hepatic arteries and then radiographed on X-ray apparatus. The results were summarized as follow ; 1. The hepatic arteries were divided into the Ramus (R.) sinister, R. dexter and R. intermedius. The intrahepatic arteries were derived from the R. sinister and R. dexter. The R. intermedius divided into the Arteria(A.) gastrica dextra, A. gastroduodenalis and A. cystica. 2. The right branch (ramus dexter) of the hepatic artery supplies the right lobe and caudate process. It consisted of the A. dorsalis lobi dextri, A. ventralis lobi dextri and A. lobi caudati. They formed one common trunk with three arteries(6 cases, 20%), and two arteries formed common trunk with the A. ventralis lobi dextri and A. lobi caudati (16 cases, 52.8%), or with A. dorsalis lobi dextri and A. lobi caudati (5 cases, 16.5%). The three arteries arose from the A. hepatia independently(3 cases, 10%). 3. The left branch (ramus sinister), larger than the right and often double (6 cases, 20%), supplies the caudate, quadrate and left lobes, and often gives origin to the A. gastrica dextra. 4. The branches of hepatic artery in the left lobe were derived from A. dorsalis lobi sinistri, A. ventralis lobi sinistri and A. intermedius lobi sinistri. The A. intermedius lobi sinistri were absent in some cases (3 cases, 10%). They almostly originated a single branch and often two branches. 5. The A. cystica arose from the R. intermedius(27 cases, 90%) and A. hepaica(3 cases, 10%). 6. The Rami processus papillarum arose from dorsal border of the Pars transversa of the left branch(19 cases, 62.7%), the left branch and right branch (9 cases, 30%) or A. hepatica(2 cases, 6.6%). 7. The A. lobi quadrata arose from either the Pars transversa of left branch (12 cases, 40%) or A. hepatica(4 cases, 13.2%). It also arose from both Pars transversa of left branch and A. ventralis lobi sinistri (3 cases, 10%). 8. The anastomosis on the branches of A. hepatica was observed in intrahepatic and cystic arteries. The left and right branches ramified several secondary radiating branches within the liver. 9. The hepatic arteries formed a very short common trunk of the right branch ($18.75{\pm}11.89$ : 2.20~44.8mm) and a long Pars transversa of the left branch($72.85{\pm}20.04$ : 28.2~104.1mm). 10. The ramified angles at the A. dorsalis lobi dextri, A. ventralis lobi dextri, A. lobi sinistri, A. ventralis lobi sinistri, A. lobi quadrata, A. cystica and Rami processus papillarum were 50-80, 270-300, 340-20, 120-160, 160-290, 200-230, 250~290, 230~280 and 80~120 degrees, respectively.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2010년도 제39회 하계학술대회 초록집
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• pp.153-153
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• 2010

Recently, to develop GaN-based light-emitting diodes (LEDs) with better performances, various approaches have been suggested by many research groups. In particular, using the patterned sapphire substrate technique has shown the improvement in both internal quantum efficiency and light extraction properties of GaN-based LEDs. In this paper, we discuss the influences of the direction of the hexagonal-structure arrays of lens-shaped patterns (HSAPs) formed on sapphire substrates on the crystal, optical, and electrical properties of InGaN/GaN multi-quantum-well (MQW) LEDs. The basic direction of the HSAPs is normal (HSAPN) with respect to the primary flat zone of a c-plane sapphire substrate. Another HSAP tilted by 30o (HSAP30) from the HSAPN structure was used to investigate the effects of the pattern direction. The full width at half maximums (FWHMs) of the double-crystal x-ray diffraction (DCXRD) spectrum for the (0002) and (1-102) planes of the HSAPN are 320.4 and 381.6 arcsecs., respectively, which are relatively narrower compared to those of the HSP30. The photoluminescence intensity for the HSAPN structure was ~1.2 times stronger than that for the HSAP30. From the electroluminescence (EL) measurements, the intensity for both structures are almost similar. In addition, the effects of the area of the individual lens pattern consisting of the hexagonal-structure arrays are discussed using the concept of the planar area fraction (PAF) defined as the following equation; PAF = [1-(patterns area/total unit areas)] For the relatively small PAF region up to 0.494, the influences of the HSAP direction on the LED characteristics were significant. However, the direction effects of the HSAP became small with increasing the PAF.

• 한국재료학회지
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• 제21권4호
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• pp.216-219
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• 2011

Perovskite manganites such as $RE_{1-x}A_xMnO_3$ (RE = rare earth, A = Ca, Sr, Ba) have been the subject of intense research in the last few years, ever since the discovery that these systems demonstrate colossal magnetoresistance (CMR). The CMR is usually explained with the double-exchange (DE) mechanism, and CMR materials have potential applications for magnetic switching, recording devices, and more. However, the intrinsic CMR effect is usually found under the conditions of a magnetic field of several Teslas and a narrow temperature range near the Curie temperature ($T_c$). This magnetic field and temperature range make practical applications impossible. Recently, another type of MR, called the low-field magnetoresistance(LFMR), has also been a research focus. This MR is typically found in polycrystalline half-metallic ferromagnets, and is associated with the spin-dependent charge transport across grain boundaries. Composites with compositions $La_{0.7}(Ca_{1-x}Sr_x)_{0.3}MnO_3)]_{0.99}/(BaTiO_3)_{0.01}$ $[(LCSMO)_{0.99}/(BTO)_{0.01}]$were prepared with different Sr doping levels x by a standard ceramic technique, and their electrical transport and magnetoresistance (MR) properties were investigated. The structure and morphology of the composites were studied by X-ray diffraction (XRD) and scanning electronic microscopy (SEM). BTO peaks could not be found in the XRD pattern because the amount of BTO in the composites was too small. As the content of x decreased, the crystal structure changed from orthorhombic to rhombohedral. This change can be explained by the fact that the crystal structure of pure LCMO is orthorhombic and the crystal structure of pure LSMO is rhombohedral. The SEM results indicate that LCSMO and BTO coexist in the composites and BTO mostly segregates at the grain boundaries of LCSMO, which are in accordance with the results of the magnetic measurements. The resistivity of all the composites was measured in the range of 90-400K at 0T, 0.5T magnetic field. The result indicates that the MR of the composites increases systematically as the Ca concentration increases, although the transition temperature $T_c$ shifts to a lower range.

• 한국결정성장학회지
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• 제14권6호
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• pp.244-252
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• 2004

$CuISe_2$ 단결정 박막은 수평 전기로에서 합성한 $CuInSe_2$ 다결정을 증발원으로하여, hot wall epitaxy(HWE) 방법으로 증발원과 기판(반절연성-GaAs(100))의 온도를 각각 $620^{\circ}C$, $410^{\circ}C$로 고정하여 단결정 박막을 성장하였다. 이때 단결정 박막의 결정성은 광발광 스펙트럼과 이중결정 선 요동곡선(DCRC) 으로 부터 구하였다. Hall 효과는 van der Pauw 방법에 의해 측정되었으며, 293K에서 운반자 농도와 이동도는 각각 $9.62\times10^{16}/\textrm{cm}^3$, 296 $\textrm{cm}^2$/Vㆍs 였다. $CuAlSe_2$/Si(Semi-Insulated) GaAs(100) 단결정 박막의 광흡수와 광전류 spectra를 293k에서 10K까지 측정하였다. 광흡수 스펙트럼으로부터 band gap $E_g$(T)는 Varshni 공식에 따라 계산한 결과 1.1851 eV-($8.99\times10^{-4} eV/K)T^2$/(T+153k)였다. 광전류 스펙트럼으로 부터 Hamilton matrix(Hopfield quasicubic mode)법으로 계산한 결과 crystal field splitting Δcr값이 0.0087eV이며 spin-orbit Δso값은 0.2329 eV임을 확인하였다. 10K일 때 광전류 봉우리들은 n = 1일때 $A_1-, B_1$-와 $C_1$-exciton봉우리임을 알았다.

• 센서학회지
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• 제13권2호
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• pp.157-167
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• 2004

A stoichiometric mixture of evaporating materials for $CuAlSe_{2}$ single crystal thin films was prepared from horizontal electric furnace. To obtain the single crystal thin films, $CuAlSe_{2}$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the hot wall epitaxy (HWE) system. The source and substrate temperatures were $680^{\circ}C$ and $410^{\circ}C$, respectively. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $CuAlSe_{2}$ single crystal thin films measured with Hall effect by van der Pauw method are $9.24{\times}10^{16}cm^{-3}$ and $295cm^{2}/V{\codt}s$ at 293 K, respectively. The temperature dependence of the energy band gap of the $CuAlSe_{2}$ obtained from the absorption spectra was well described by the Varshni's relation, $E_{g}(T)$ = 2.8382 eV - ($8.68{\circ}10^{-4}$ eV/K)$T^{2}$/(T + 155 K). The crystal field and the spin-orbit splitting energies for the valence band of the $CuAlSe_{2}$ have been estimated to be 0.2026 eV and 0.2165 eV at 10 K, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the ${\Delta}so$ definitely exists in the ${\Gamma}_{5}$ states of the valence band of the $CuAlSe_{2}$. The three photocurrent peaks observed at 10 K are ascribed to the $A_{1-}$, $B_{1-}$, and $C_{1-}$ exciton peaks for n = 1.

• 센서학회지
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• 제23권2호
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• pp.134-141
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• 2014

A stoichiometric mixture of evaporating materials for $BaIn_2Se_4$ epilayers was prepared from horizontal electric furnace. To obtain the single crystal thin films, $BaIn_2Se_4$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the Hot Wall Epitaxy (HWE) system. The source and substrate temperatures were $620^{\circ}C$ and $400^{\circ}C$, respectively. The crystalline structure of the epilayers was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $BaIn_2Se_4$ epilayers measured from Hall effect by van der Pauw method are $8.94{\times}10^{17}cm^{-3}$ and 343 $cm^2/vs$ at 293 K, respectively. The temperature dependence of the energy band gap of the $BaIn_2Se_4$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)$=2.6261 eV-$(4.9825{\times}10^{-3}eV/K)T^2/(T+558 K)$. The crystal field and the spin-orbit splitting energies for the valence band of the $BaIn_2Se_4$ have been estimated to be 116 meV and 175.9 meV, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the ${\Delta}so$ definitely exists in the ${\Gamma}_5$ states of the valence band of the $BaIn_2Se_4/GaAs$ epilayer. The three photocurrent peaks observed at 10 K are ascribed to the $A_1-$, $B_1$-exciton for n = 1 and $C_{21}$-exciton peaks for n=21.

• 한국결정학회지
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• 제12권4호
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• pp.197-206
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• 2001

수평 전기로에서 AgInS₂ 다결정을 합성하여 HWE(Hot Wall Epitaxy)방법으로 AgInS₂ 단결정 박막을 반절연성 GaAs(100)기판에 성장시켰다. AgInS₂ 단결정 박막의 성장 조건은 증발원의 온도 680℃, 기판의 온도 410℃였고 성장 속도는 0.5㎛/hr였다. AgInS₂ 단결정 박막의 결정성의 조사에서 10 K에서 광발광(photoluminescence)스펙트럼이 597.8 nm(2.0741 eV)에서 exciton emission스펙트럼이 가장 강하게 나타났으며, 또한 이중결정 X-선 요동곡선(DCRC)의 박폭치(FWHM)도 121 arcsec로 가장 작아 최적 성장 조건임을 알수 있었다. Hall 효과는 van der Pauw 방법에 의해 측정되었으며, 온도에 의존하는 운반자 농도와 이동도는 293K에서 각각 9.35×10/sup 16/㎤, 294㎠/V·s 였다. AgInS₂ /SI(SEmi-Insulated) GaAs(100) 단결정 박막의 광흡수와 광전류 spectra를 293K에서 10K까지 측정하였다. 광흡수 스펙트럼으로부터 band gap E/sub g/(T)는 Varshni 공식에 따라 계산한 결과 2.1365eV-(9.89×10/sup-3/eV/K/)T²(T+2930K)이었으며 광전류 스펙트럼으로부터 Hamiltopn matrix(Hopfield quasicubic mode)법으로 계산한 결과 crystal field splitting Δcr값이 0.1541eV이며 spin-orbit Δso 값은 0.0129eV임을 확인하였다. 10K일때 광전류 봉우리들은 n=1 일때 A₁-, B-₁와 C₁-exction 봉우림을 알았다.

• 센서학회지
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• 제24권6호
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• pp.404-411
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• 2015

A stoichiometric mixture of evaporating materials for $BaAl_2Se_4$ single crystal thin films was prepared from horizontal electric furnace. To obtain the single crystal thin films, $BaAl_2Se_4$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the Hot Wall Epitaxy (HWE) system. The source and substrate temperatures were $610^{\circ}C$ and $410^{\circ}C$, respectively. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $BaAl_2Se_4$ single crystal thin films measured from Hall effect by van der Pauw method are $8.29{\times}10^{-16}cm^{-3}$ and $278cm^2/vs$ at 293 K, respectively. The temperature dependence of the energy band gap of the $BaAl_2Se_4$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)=3.4205eV-(4.3112{\times}10^{-4}eV/K)T^2/(T+232 K)$. The crystal field and the spin-orbit splitting energies for the valence band of the $BaAl_2Se_4$ have been estimated to be 249.4 meV and 263.4 meV, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the ${\Delta}so$ definitely exists in the ${\Gamma}_5$ states of the valence band of the $BaAl_2Se_4/GaAs$ epilayer. The three photocurrent peaks observed at 10 K are ascribed to the $A_1$-, $B_1$-exciton for n =1 and $C_{31}$-exciton peaks for n=31.