• 한국재료학회지
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• 제18권4호
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• pp.222-227
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• 2008

In this study, $BaTiO_3$ thin films were grown by RF-magnetron sputtering, and the effects of a post-annealing process on the structural characteristics of the $BaTiO_3$ thin films were investigated. For the crystallization of the grown thin films, post-annealing was carried out in air at an annealing temperature that varied from $500-1000^{\circ}C$. XRD results showed that the highest crystal quality was obtained from the samples annealed at $600-700^{\circ}C$. From the SEM analysis, no crystal grains were observed after annealing at temperatures ranging from 500 to $600^{\circ}C$; and 80 nm grains were obtained at $700^{\circ}C$. The surface roughness of the $BaTiO_3$ thin films from AFM measurements and the crystal quality from Raman analysis also showed that the optimum annealing temperature was $700^{\circ}C$. XPS results demonstrated that the binding energy of each element of the thin-film-type $BaTiO_3$ in this study shifted with the annealing temperature. Additionally, a Ti-rich phenomenon was observed for samples annealed at $1000^{\circ}C$. Depth-profiling analysis through a GDS (glow discharge spectrometer) showed that a stoichiometric composition could be obtained when the annealing temperature was in the range of 500 to $700^{\circ}C$. All of the results obtained in this study clearly demonstrate that an annealing temperature of $700^{\circ}C$ results in optimal structural properties of $BaTiO_3$ thin films in terms of their crystal quality, surface roughness, and composition.

• 한국진공학회지
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• 제17권4호
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• pp.365-373
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• 2008

최적화된 량의 황화수소 첨가 가스를 이용하여 실리콘 기판위에 증착된 Fe/Al 박막위에 촉매 화학 기상 증착법을 사용하여 직경이 얇은 다중층 탄소나노튜브가 수직 정렬되어 합성되었다. 주사전자현미경 관측 이미지에서 합성된 탄소나노튜브는 상대적으로 일정한 길이를 가지고 기판에 수직으로 정렬되었다. 투과전자현미경 관측에서 합성된 탄소나노튜브는 10nm 이내의 작은 외경을 가졌고 촉매가 거의 없었다. 평균 튜브의 벽 수는 약 다섯 개이다. 수직 정렬된 직경이 얇은 다중층 탄소나노튜브의 성장 메카니즘이 제시되었다. 수직 정렬된 직경이 얇은 다중층 탄소나노튜브는 $0.1\;{\mu}A/cm^2$의 전류밀도에서 약 $1.1\;V/{\mu}m$ 낮은 턴-온 전계를 나타내었고 $2.7\;V/{\mu}m$의 전계에서 약 $2.5\;mA/cm^2$의 전류밀도를 얻었다. 게다가, 수직 정렬된 직경이 얇은 다중층 탄소나노튜브는 약 $1\;mA/cm^2$의 전류밀도에서 20시간동안 전류밀도 저하 없이 좋은 전계 방출 안정성을 보여주었다.

• 한국재료학회지
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• 제13권8호
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• pp.519-523
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• 2003

We report the synthesis of cubic spinel $ZnCo_2$$O_4$thin films and the tunability of the conduction type by control of the oxygen partial pressure ratio. Zinc cobalt oxide films were grown on$ SiO_2$(200 nm)/Si substrates by reactive magnetron sputtering method using Zn and Co metal targets in a mixed Ar/$O_2$atmosphere. We found from X-ray diffraction measurements that the crystal structure of the zinc cobalt oxide films grown under an oxygen-rich condition (the $O_2$/Ar partial pressure ratio of 9/1) changes from wurtzite-type $Zn_{1-x}$ $Co_{X}$O to spinel-type $ZnCo_2$$O_4$with the increase of the Co/Zn sputtering ratio,$ D_{co}$ $D_{zn}$ . We noted that the above structural change accompanied by the variation of the majority electrical conduction type from n-type (electrons) to p-type (holes). For a fixed $D_{co}$ $D_{zn}$ / of 2.0 yielding homogeneous spinel-type $_2$O$ZnCo_4$films, the type of the majority carriers also varied, depending on the$ O_2$/Ar partial pressure ratio: p-type for an $O_2$-rich and n-type for an Ar-rich atmosphere. The maximum electron and hole concentrations for the Zn $Co_2$ $O_4$films were found to be 1.37${\times}$10$^{20}$ c $m^{-3}$ and 2.41${\times}$10$^{20}$ c $m^{-3}$ , respectively, with a mobility of about 0.2 $\textrm{cm}^2$/Vs and a high conductivity of about 1.8 Ω/$cm^{-1}$ /.

• 마이크로전자및패키징학회지
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• 제19권2호
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• pp.67-72
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• 2012

최근에 전자 산업 분야에서 장치의 고용량을 구현 하기 위해 구동 drive IC의 선폭은 좁아지고 집적도는 증가하고 있다. 이러한 반도체, 전자 산업 분야의 초소형화, 고밀도화에 따라 FCCL(Flexible Copper Clad Laminate)의 표면 품질이 더욱 중요해 지고 있다. FCCL의 표면 결함으로는 돌기, 스크레치, 덴트 등이 있다. 특히 돌기가 표면에 존재할 경우 후속 공정에서 쇼트와 같은 불량을 유발할 수 있으며, 제품의 품질 저하를 야기 시킬 수 있다. 하지만 표면에 돌기가 존재한다 하더라도, 전해액의 레벨링 특성이 우수하다면 돌기의 성장을 막을 수 있다.평탄하고, 결함이 없는 도금표면을 얻기 위해서는 첨가제의 역할이 필수적이다. 평탄한 구리 표면을 형성하기 위해서 stock solution에 가속제, 억제제, 레벨러를 첨가하였다. 레벨러를 첨가하는 이유는 평탄한 표면을 얻고, 돌기의 형성을 억제하기 위함이다. 구리도금 표면 형상을 향상시키기 위한 레벨러로는 SO(Safranin O), MV(Methylene Violet), AB(Alcian Blue), JGB(Janus Green B), DB(Diazine Black) and PVP(Polyvinyl Pyrrolidone)가 사용되었다. 도금 첨가제와 도금 조건의 변화를 통해 도금시레벨링 특성을 향상시키고, 레벨링 특성 측정을 위해 니켈 인공돌기를 제작 한 후 레벨링 특성을 측정하였다.

• 한국전기전자재료학회논문지
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• 제33권3호
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• pp.214-218
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• 2020

In this study, Mg_xZn_1-xO thin films, which can be applied not only to active layers of light-emitting devices (LEDs), such as UV-LEDs, but also to solar cells, high mobility field-effect transistors, and power semiconductor devices, are fabricated using the sol-gel method. ZnO and Mg_0.3Zn_0.7O solution synthesized by the sol-gel method and the thin film were grown by spin coating on a Si (100) substrate and sapphire substrate. The solutions are synthesized by dissolving precursor materials in 2-methoxyethanol (2-ME) solvent, and then monoethanolamine (MEA) was added to the mixed solution as a sol stabilizer. Zinc acetate dihydrate is used as a ZnO precursor, while Mg nitrate hexahydrate and Mg acetate tetrahydrate are used as an MgO precursor. Then, the optical and structural characteristics of the fabricated thin films are compared. The molar concentration of the Zn precursor in the solvent is fixed at 0.3 M, and the amount of the Mg precursor is 30% of Mg²⁺/Zn²⁺. The optical characteristics are measured using an UV-vis spectrophotometer, and the transmittance of each wavelength is measured. Structural characteristics are measured using X-ray diffraction (XRD) and transmission electron microscopy (TEM). Composition analyses are performed using energy dispersive X-ray spectroscopy (EDS). The Mg_0.3Zn_0.7O thin film was well formed at the ratio of the Mg precursor added regardless of the type of Mg precursor, and the c-axis of the thin film was decreased, while the band gap was increased to 3.56 eV.

• 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.

• 한국재료학회지
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• 제21권11호
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• pp.634-638
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• 2011

We report growth of epitaxial AlN thin films on c-plane sapphire substrates by plasma-assisted molecular beam epitaxy. To achieve two-dimensional growth the substrates were nitrided by nitrogen plasma prior to the AlN growth, which resulted in the formation of a two-dimensional single crystalline AlN layer. The formation of the two-dimensional AlN layer by the nitridation process was confirmed by the observation of streaky reflection high energy electron diffraction (RHEED) patterns. The growth of AlN thin films was performed on the nitrided AlN layer by changing the Al beam flux with the fixed nitrogen flux at 860$^{\circ}C$. The growth mode of AlN films was also affected by the beam flux. By increasing the Al beam flux, two-dimensional growth of AlN films was favored, and a very flat surface with a root mean square roughness of 0.196 nm (for the 2 ${\mu}m$ ${\times}$ 2 ${\mu}m$ area) was obtained. Interestingly, additional diffraction lines were observed for the two-dimensionally grown AlN films, which were probably caused by the Al adlayer, which was similar to a report of Ga adlayer in the two-dimensional growth of GaN. Al droplets were observed in the sample grown with a higher Al beam flux after cooling to room temperature, which resulted from the excessive Al flux.

• 공업화학
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• 제30권4호
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• pp.499-503
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• 2019

GaInP/GaAs 양자우물(quantum well)구조를 N-AlGaInP/p-GaInP 이종 접합구조 태양전지에 도입하여 그 특성을 조사하고 양자우물구조가 없는 태양전지와 비교하였다. 에피층은 (100)평면이 (111)A 방향으로 $6^{\circ}$ 기울어진 p-GaAs 기판 위에 성장하였다. 태양전지 박막구조는 두께 400 nm의 N-AlGaInP 층에 590 nm의 p-GaInP와 210 nm의 GaInP/GaAs 양자 우물 구조(10 nm GaInP/5 nm GaAs의 14겹 구조)가 도입된 양자우물 태양전지 구조와 800 nm의 p-GaInP의 단일이종접합 구조로 이루어진다. 측정결과 $1{\times}1mm^2$의 태양전지에서 단락전류밀도($J_{sc}$)는 양자우물구조가 도입된 태양전지에서는 $9.61mA/cm^2$, 양자우물 구조가 없는 태양전지에서는 $7.06mA/cm^2$가 각각 측정되었다. 이차이온질량 분석법(SIMS)과 외부양자효율(external quantum efficiency) 측정을 통하여 단락전류 증가에 의한 효율증가가 흡수 스펙트럼의 확대가 아닌 양자우물에 의한 carrier 재결합의 억제에 의한 효과임을 확인하였다.

• Korean Chemical Engineering Research
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• 제57권1호
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• pp.111-117
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• 2019

기상으로 전달된 Ti 전구체가 열 플라즈마에서 고순도의 결정질 코어-$TiO_2$로 합성됨과 동시에 기판에 바로 증착시킬 수 있는 공정을 제시한다. 제조된 코어-$TiO_2$는 외부에 노출되지 않는 상태에서 원자층증착법(Atomic Layer Deposition, ALD)에 의하여 $Al_2O_3$로 코팅된다. 코어-$TiO_2$와 코팅된 쉘-$Al_2O_3$의 형태학적 특징은 transmission electron microscope (TEM) 및 transmission electron microscope - energy dispersive spectroscopy (TEM-EDS)를 통해 분석하였다. 제조된 코어-$TiO_2$/쉘-$Al_2O_3$ 나노입자의 전기적 특성은 염료감응 태양전지(dye-sensitized solar cell, DSSC)의 작동전극에 적용하여 평가하였다. Dynamic light scattering system (DLS), scanning electron microscope (SEM), X-ray Diffraction (XRD)을 통하여 코어-$TiO_2$의 평균입도, 성장속도 및 결정구조의 무게분율을 분석한 결과, 평균입도는 17.1 nm, 코어박막의 두께는 $20.1{\mu}m$이고 주 결정구조가 Anatase로 증착된 코어-$TiO_2$/쉘-$Al_2O_3$ 나노입자를 적용한 DSSC가 기존의 페이스트 방식으로 제작한 DSSC보다 더 높은 광효율을 보여준다. 기존의 페이스트방식을 활용한 DSSC의 에너지변환효율 4.99%에 비하여 선택적으로 조절된 코어-$TiO_2$/쉘-$Al_2O_3$ 나노입자를 작동전극으로 사용한 경우가 6.28%로 26.1% 더 높은 광효율을 보여준다.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2003년도 춘계학술발표강연 및 논문개요집
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• pp.81-81
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• 2003

The stochiometric mixture of evaporating materials for the CuGaSe$_2$ single crystal thin films were prepared from horizontal furnace. Using extrapolation method of X-ray diffraction patterns for the polycrystal CuGaSe$_2$, it was found tetragonal structure whose lattice constant no and co were 5.615$\AA$ and 11.025$\AA$, respectively. To obtains the single crystal thin films, CuGaSe$_2$ mixed crystal was deposited on throughly etched GaAs(100) by the Hot Wall Epitaxy(HWE) system. The source and substrate temperature were 61$0^{\circ}C$ and 45$0^{\circ}C$ respectively, and the growth rate of the single crystal thin films was about 0.5${\mu}{\textrm}{m}$/h. The crystalline structure of single crystal thin films was investigated by the double crystal X-ray diffraction(DCXD). Hall effect on this sample was measured by the method of van der pauw and studied on carrier density and mobility depending on temperature. From Hall data, the mobility was likely to be decreased by pizoelectric scattering in the temperature range 30K to 150K and by polar optical scattering in the temperature range 150K to 293K. The optical energy gaps were found to be 1.68eV for CuGaSe$_2$ single crystal thin films at room temperature. The temperature dependence of the photocurrent peak energy is well explained by the Varshni equation then the constants in the Varshni equation are given by a=9.615$\times$ 10$^{-4}$ eV/K, and $\beta$=335K. From the photocurrent spectra by illumination of polarized light of the CuGaSe$_2$ single crystal thin films. We have found that values of spin orbit coupling ΔSo and crystal field splitting ΔCr was 0.0900eV and 0.2498eV, respectively. From the PL spectra at 20K, the peaks corresponding to free bound excitons and D-A pair and a broad emission band due to SA is identified. The binding energy of the free excitons are determined to be 0.0626eV and the dissipation energy of the acceptor-bound exciton and donor-bound exciton to be 0.0352eV, 0.0932eV, respectively.