• E2M - 전기 전자와 첨단 소재
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• 제9권8호
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• pp.789-798
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• 1996

The double nitride layer Metal Nitride Oxide Semiconductor(MNOS) structures were fabricated by variating both gas ratio and nitride thickness, and by duplicating nitride deposited and one nitride layer MNOS structure to improve nonvolatile memory characteristics of MNOS structures by Low Pressure Chemical Vapor Deposition(LPCVD) method. The nonvolatile memory characteristics of write-in, erase, memory retention and degradation of Bias Temperature Stress(BTS) were investigated by the homemade automatic .DELTA. $V_{FB}$ measuring system. In the trap density double nitride layer structures were higher by 0.85*10$^{16}$ $m^{-2}$ than one nitride layer structure, and the AVFB with oxide field was linearly increased. However, one nitride layer structure was linearly increased and saturated above 9.07*10$^{8}$ V/m in oxide field. In the erase behavior, the hole injection from silicon instead of the trapped electron emission was observed, and also it was highly dependent upon the pulse amplitude and the pulse width. In the memory retentivity, double nitrite layer structures were superior to one nitride layer structure, and the decay rate of the trapped electron with increasing temperature was low. At increasing the number on BTS, the variance of AVFB of the double nitride layer structures was smaller than that of one nitride layer structure, and the trapped electron retention rate was high. In this paper, the double nitride layer structures were turned out to be useful in improving the nonvolatile memory characteristics.

• 대한기계학회논문집B
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• 제35권4호
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• pp.337-344
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• 2011

고분자 전해질막 연료전지에서 공급 기체의 가습은 연료전지의 효율과 수명 향상 측면에서 필수적이다. 기존의 고분자 전해질막 연료전지의 가습 방법으로 물 분사나 막가습기, 엔탈피 휠 등이 사용되었다. 하지만, 이러한 외부 가습 방법은 시스템 부피를 크게 하고 고출력 구간에서 가습량이 부족한 단점이 있다. 가습 장치의 효율과 전체 연료전지 시스템 효율을 높이려면, 연료전지의 고온다습한 배출기체로부터 열과 수분을 회수할 필요가 있다. 본 연구에서는 연료전지의 고온다습한 배출공기를 재순환하여 공급공기를 1 차로 가습하고 소형의 막가습기로 2 차 가습하는 복합가습에 대한 해석적 연구를 수행하였다. 그리고 최적의 가습 시스템 설계를 위한 새로운 방법을 제안하였다.

• Journal of Advanced Marine Engineering and Technology
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• 제32권5호
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• pp.707-716
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• 2008

The objective of this study was to analyze the effect of mixed fuel composition and mass fraction on spray inner structure in evaporating transient spray under the variant ambient conditions. Spray structure and spatial distribution of liquid phase concentration were investigated using a thin laser sheet illumination technique on the three component mixed fuels. A pulsed Nd:YAG laser was used as a light source. The experiments were conducted in a constant volume vessel with optical access. Fuel was injected into the vessel with electronically controlled common rail injector. Used fuel contains i-octane($C_8H_{18}$), n-dodecane($C_{12}H_{26}$) and n-hexadecane($C_{16}H_{34}$) that were selected as low-, middle- and high-boiling point fuel, respectively. Experimental conditions are 42 MPa, 72 MPa and 112 MPa in injection pressure, $5\;kg/m^3$, $15kg/m^3$ and $30kg/m^3$ in ambient gas density, 300 K, 500 K, 600 K and 700 K in ambient gas temperature, 300 K and 368 K in fuel temperature and different fuel mass fraction. Experimental results indicated that the multi-component fuels made two phase region mixed vapor and liquid so that it would are helpful to improve combustion, for the fuels of high boiling point component could accelerate evaporation very much according as low boiling point fuel was added to high boiling point fuel.

• 한국대기환경학회지
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• 제28권1호
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• pp.39-51
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• 2012

Aerosol slurry samples were collected in 60-min interval using Korean Semi-continuous Elements in Aerosol Sampler (KSEAS) between May 19 and June 6, 2010 at an urban site of Gwangju. The $PM_{2.5}$ samples were collected with a flow rate of 16.7 L/min and particles are grown by condensation of water vapor in a condenser maintained at ${\sim}5^{\circ}C$ after saturation by direct injection of steam. The resulting droplets are collected in a liquid slurry with a airdroplet separator. Concentrations of 16 elements (Al, Fe, Mn, Ca, K, Cu, Zn, Pb, Cd, Cr, Ti, V, Ni, Co, As, Se) in the collected slurry samples were determined off-line by ICP-MS. KSEAS sample analysis encompassed the sampling periods for which 24-hr average elemental species concentrations were calculated for comparison with those derived from 24-hr integrated filter samples. Relationship between elemental species measured by two methods indicated high correlation coefficients (r), mostly greater than r of 0.80. However, we note that concentrations of Al, K, Ca, Mn, and Fe, which are often associated with crustal elemental particles, in the KSEAS samples, were substantially lower (1.4~11 times) than those found in the typical filter-based samples. This discrepancy is probably due to difficulties in transferring insoluble dust particles to the collection vials in the KSEAS. Temporal profiles of elemental concentrations indicate that some transient events in their concentrations are observed over the sampling periods. For the elemental species studied, atmospheric concentrations during the transient events increased by factors of 4 in Mn~80 in Zn, compared to their background levels. Principle component analyses were applied to the hourly KSEAS data sets to identify sources affecting the concentrations of the metal constituents observed. In this study, we conclude that hourly measurements for particle-bound elemental constituents were extremely useful for revealing the short-term variability in their concentrations and developing insights into their sources.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.490-490
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• 2011

Graphene, hexagonal network of carbon atoms forming a one-atom thick planar sheet, has been emerged as a fascinating material for future nanoelectronics. Huge attention has been captured by its extraordinary electronic properties, such as bipolar conductance, half integer quantum Hall effect at room temperature, ballistic transport over ${\sim}0.4{\mu}m$ length and extremely high carrier mobility at room temperature. Several approaches have been developed to produce graphene, such as micromechanical cleavage of highly ordered pyrolytic graphite using adhesive tape, chemical reduction of exfoliated graphite oxide, epitaxial growth of graphene on SiC and single crystalline metal substrate, and chemical vapor deposition (CVD) synthesis. In particular, direct synthesis of graphene using metal catalytic substrate in CVD process provides a new way to large-scale production of graphene film for realization of graphene-based electronics. In this method, metal catalytic substrates including Ni and Cu have been used for CVD synthesis of graphene. There are two proposed mechanism of graphene synthesis: carbon diffusion and precipitation for graphene synthesized on Ni, and surface adsorption for graphene synthesized on Cu, namely, self-limiting growth mechanism, which can be divided by difference of carbon solubility of the metals. Here we present that large area, uniform, and layer controllable graphene synthesized on Cu catalytic substrate is achieved by acetylene-assisted CVD. The number of graphene layer can be simply controlled by adjusting acetylene injection time, verified by Raman spectroscopy. Structural features and full details of mechanism for the growth of layer controllable graphene on Cu were systematically explored by transmission electron microscopy, atomic force microscopy, and secondary ion mass spectroscopy.

• Nuclear Engineering and Technology
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• 제48권2호
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• pp.457-469
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• 2016

During the late phase of severe accidents of light water reactors, a porous debris bed is expected to develop on the bottom of the flooded reactor cavity after breakup of the melt in water. The geometrical configuration, i.e., internal and external characteristics, of the debris bed is significant for the adequate assessment of the coolability of the relocated corium. The internal structure of a debris bed was investigated experimentally using the DAVINCI (Debris bed research Apparatus for Validation of the bubble-Induced Natural Convection effect Issue) test facility. Particle sedimentation under the influence of a two-phase natural convection flow due to the decay heat in the debris bed was simulated by dropping various sizes of particles into a water vessel with air bubble injection from the bottom. Settled particles were collected and sieved to obtain the particle mass, size distribution in the radial and axial positions, and the bed porosity and permeability. The experimental results showed that the center part of the particle bed tended to have larger particles than the peripheral area. For the axial distribution, the lower layer had a higher fraction of larger particles. As the sedimentation progressed, the size distribution in the upper layers can shift to larger sizes because of the higher vapor generation rate and stronger flow intensity.

• Applied Science and Convergence Technology
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• 제26권4호
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• pp.79-85
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• 2017

The crack-free AlGaN template has been successfully grown by using selective area growth with triangular GaN facet. The triangular GaN stripe structure was obtained by vertical growth rate enhanced mode with low growth temperature of $950^{\circ}C$ and high growth pressure of 500 torr. The lateral growth rate enhanced mode of AlGaN for crack-free and flat surface was also investigated. Low pressure of 30 torr and high V/III ratio of 4400 were favorable for lateral growth of AlGaN. It was confirmed that the $4{\mu}m$ -thick $Al_{0.2}Ga_{0.8}N$ was crack-free over entire 2-inch wafer. The dislocation density of $Al_{0.2}Ga_{0.8}N$ was as low as ${\sim}7.6{\times}10^8/cm^2$ measured by cathodoluminescence. Based on the high quality AlGaN with low dislocation density, the ultraviolet laser diode epitaxy with cladding, waveguide and GaN/AlGaN multiple quantum well (MQW) was grown by metalorganic chemical vapor deposition. The stimulated emission at 349 nm with full width at half maximum of 1.8 nm from the MQW was observed through optical pumping experiment with 193 nm KrF laser. We also have fabricated the deep ridge type ultraviolet laser diode (UV-LD) with $5{\mu}m-wide$ and $700{\mu}m-long$ cavity for electrical properties. The turn on voltage was below 5 V and the resistance was ${\sim}55{\Omega}$ at applied voltage of 10 V. The amplified spontaneous emission spectrum of UV-LD was also observed from pulsed current injection.

• 한국지하수토양환경학회지:지하수토양환경
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• 제9권2호
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• pp.28-40
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• 2004

토양증기추출(Soil Vapor Extraction)법을 이용하여 대표적 휘발성 오염물질(VOCs)인 가솔린을 토양으로부터 제거하는 박스실험을 실시하였다. 아크릴수지로 제작된 65 cm${\times}$20 cm${\times}$30 cm 규모의 박스를 제작하여, 인공적인 토양 환경을 설정한 후, 직경 1 cm인 스테인레스 재질의 관에 0.2cm 간격으로 하부에서 15cm까지 스크린 된 스테인레스 재질의 주입정(2개)과 추출정(1개)을 설치하여 SVE를 실시하였으며, 추출정으로부터 배출되는 가스를 제거하는 후처리 공정을 연결하여 SVE로부터 배출되는 가스의 가솔린 농도와 후처리 공정 후 배출되는 가솔린 농도를 비교 분석하였다. 가솔린 100g을 토양 내 주입한 경우 0.03 L/min 조건의 박스실험에서는 SVE에 의해 약 560L (13일 경과) 가스 추출 후 주입된 가솔린의 95%가 제거되었으며, 주입 가솔린양이 250 g이고 추출 가스량이 0.2 L/min 조건에서는 약 1440L(5일 경과)가스 추출 후 주입 가솔린의 92% 이상이 제거되어, SVE가 토양 내 휘발성 오염물질을 제거하는데 매우 효과적인 방법임을 입증하였다. 가솔린으로 오염된 토양에서 SVE 공정으로부터 배출되는 가스를 과립상 활성탄 흡착탑과 바이오필터를 이용하여 제거하는 실험을 실시하였다. SVE로부터 배출된 가스의 후처리 공정으로 활성탄의 흡착탑을 이용한 제거 공정과 바이오필터를 이용한 제거 공정의 효율을, 후처리 공정으로 주입되는 가스내 가솔린량에 대한 운전 시간별 제거 효율로 나타내었다. 제거 효율은 후처리 공정에 주입되는 가솔린의 농도와 관계 없이 평균 94%의 높고 안정적인 효율을 나타내었고, 후처리 후 배출되는 가스의 농도 자체도 매우 낮게 나타남으로서, 실제 오염지역에서 토양증기추출법과 결합 된 하나의 VOCs 제거공정으로서 효과적으로 사용될 수 있음을 입증하였다. 활성탄 흡착탑과 바이오필터에 유입되는 가솔린의 부하량에 대한 제거 용량은, 주입되는 가솔린의 농도가 상당히 높음에도 불구하고 주입되는 가솔린의 농도가 높을수록 선형적으로 증가하였다. 이러한 결과들은 후처리 공정들이 SVE에서 배출되는 가스의 VOCs 농도가 다양한 환경에서도 광범위하게 적용할 수 있으며, 특히 고농도의 가스상을 처리하는 데에도 매우 효과적으로 사용될 수 있음을 입증한다.

• 한국결정성장학회지
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• 제19권2호
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• pp.61-65
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• 2009

본 논문에서는 형광체가 없는 백색 LED의 성장과 광학적인 특성을 분석하였다. 혼합소스(miked-source) HVPE(hydride vapor phase epitaxy) 방법과 다중성장보트를 이용하여 MOCVD로 얇게 성장한 n-GaN 위에 활성층을 AlGaN으로 한 이종접합구조(DH; Doublehetero structure)를 성장하고, 패키징 단계를 거쳐 비형광체 단일칩 백색 LED 램프를 제작하였다. 패키징 한 소자를 주입전류 $10{\sim}100mA$로 변화시켜 측정한 결과 색 연색성 값은 72-93, 색좌표의 좌표값은 X값은 $0.26{\sim}0.34$, Y값은 $0.31{\sim}0.40$에서 가지며, 색온도는 $5126{\sim}10406K$ 범위에서 측정되었다. 또한 주입전류 증가 시, 형광체를 사용한 백색 LED는 청색 영역으로 이동하지만, 제작된 백색 LED는 황색영역으로 색좌표가 이동하였다. 이러한 특성을 통하여 고감도의 색 연색성 값을 가지는 비형광체 백색LED의 성장 가능성을 확인하였으며, 광 특성 분석 결과를 통하여 혼합소스의 성장 메커니즘을 제안하고자 한다.

• Journal of Radiation Protection and Research
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• 제33권1호
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• pp.13-20
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• 2008

석유 및 정유관련 산업에서 다중상(multi-phase flow) 유체의 배관 내 흐름은 일반적인 현상의 하나이다. 그러나 각각의 상에 대한 정확한 유량측정은 항상 정확한 결과획득을 얻는데 장애의 근원으로 작용하였다. 일반 상업용 유량계는 일정 이상의 기포가 포함된 유체 흐름의 경우 유량계측에 상당한 오차를 유발한다. 본 연구에서는 ${\gamma}$-ray attenuation 기법을 이용하여 clamp-on 타입으로 배관 외부에서 다중상 유체흐름의 유량 측정을 수행하였다. 사용된 밀봉 감마선원으로는 $^{137}Cs$ 20 mCi와 17 mCi 두 개의 동위원소를 사용하였으며, 감마선 검출기로는 $2"{\times}2"$ NaI(Tl) 섬광계수관을 이용하였다. 방사선 검출기로부터 데이터를 수집하고 각각의 데이터에 대해 푸리에 변환과 필터링을 통해 노이즈를 최소화하였다. 복원된 신호에 대해 상호상관함수(cross correlation function)를 적용하여 두 검출기 사이의 통과시간(transit time)을 측정함으로써 유량을 산정하였다. 배관 내 기포함량 측정을 통해 유량을 보정해줌으로써 측정유량의 정확도를 높였다. 두 선원간의 거리가 4D(D; inner diameter) 그리고 본 실험의 측정조건(N/S: $0.12{\sim}0.15$, sampling time ${\Delta}\;t$: 4msec) 하에서 기포량(단면적 대비 $6.1\;%{\sim}9.2\;%$) 보정을 통해 산정된 유량은 계측오차가 실제 평균유량 대비 1.7 % 이하인 정확도를 보였다. 또한 두 밀봉 감마선원 간의 거리가 가까울수록 통과시간 측정에 정확도가 향상되므로 보다 정확한 유량측정이 가능하였다. 본 연구를 통해 다중상 혼합유체의 유량을 밀봉감마선원과 상호상관 기법으로 이용하여 계측할 수 있음을 확인하였다. 방사성동위원소의 선택 및 계측시스템의 최적화 조건 등에 대한 추가연구가 수행된다면 석유화학 산업과 같은 장치산업의 유지관리 측면에 경제적으로 크게 기여할 수 있을 것으로 판단된다.