• Title/Summary/Keyword: 광 조사 간격

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Comparative Analysis of Growth and Development of Paddy Rice (Oryza sativa L.) by Light Intensity under Farm-type Solar Photovoltanic Power Station (추적식 영농형 태양광발전시스템 구축에 따른 음영별 하부작물 벼(Oryza sativa L.)의 생육비교)

  • Eon-Yak Kim;Ye-Jin Lee;In-Jin Kang;Hye-Min Son;Min-Ho Shin;Chang-Hyu Bae
    • Proceedings of the Plant Resources Society of Korea Conference
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    • 2022.09a
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    • pp.85-85
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    • 2022
  • 영농형 태양광발전은 태양의 일사량을 전기발전과 영농에 공유하는(solar-sharing) 방식이다. 본 연구는 신재생에너지의 활용의 극대화를 위하여 추적식 영농형 태양광발전시스템을 구축하고 시설하부에서 일정 기간 재배중인 작물의 하부 환경과 생육을 조사하여 영농형태양광 하부작물개발을 위한 기초자료를 확보하고자 하였다. 구축한 추적식 영농형 태양광발전시스템은 4열 6단의 24장 모듈(8m × 6m)을 가지며, 발전시설 중심축 기둥 간 중심간격 14m로 단일지주식 스크루 공법으로 순천대학교 부속농장 답작포(순천시 죽평리)에 설치하여 하부 환경과 하부작물의 생육을 조사하였다. 태양광발전시설 하부작물의 생육을 조사하기 위하여 순천 농협육묘장에서 벼(신동진)를 육묘하여 2022년 6월 16일 이앙하였다. 태양광발전시스템 하부 지역을 4방위 방향에 따라 강음영(중심축으로부터 1~3m), 중음영(5m), 약음영(7~9m) 구역으로 설정하여 생육을 조사한 결과, 방위에 따른 초장은 남쪽에서 음영간 차이가 상대적으로 낮게 나타났으며, 1번기 태양광 발전시설에 의하여 음영이 중첩된 2번기 시설의 동쪽에서 대조구 대비 초장이 상대적으로 낮은 경향을 나타내었다. 음영강도에 따른 초장은 대체로 강음영구에서 낮게 나타났으며, 약음영구로 갈수록 높게 나타났다. 엽수는 방위에 따라서, 그리고 음영의 강도에 따른 차이가 초장에 비하여 작게 나타났다. 출수기의 경우 방위별로는 남쪽에서 음영별 차이가 작게 나타났으며, 음영강도에 따라서 차이를 보였다. 또한 태양광시설 하부에 데이터수집장치(Model 1650, Spctrum Technonogies, USA)를 설치하여 음영에 따른 토양전도도, 토양함수량, 토양온도, par light 등 생육환경을 조사, 비교하였다.

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Polymerization Shrinkage Distribution of a Dental Composite during Dental Restoration Observed by Digital Image Correlation Method (디지털 이미지 상관법을 이용한 치과용 복합레진의 수복 시 중합수축분포 관찰)

  • Park, Jung-Hoon;Choi, Nak-Sam
    • Composites Research
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    • v.30 no.6
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    • pp.393-398
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    • 2017
  • The shrinkage distribution of a dental composite (Clearfil AP-X, Kuraray, Japan) used for dental restoration was observed using a digital image correlation method. In order to analyze the shrinkage distribution formed during and after light irradiation, digital images were taken with different photographing conditions for each period. Optimal photographing conditions during LED irradiation were obtained through a preliminary experiment in which the exposure time was applied from 0.15 ms to 0.55 ms in 0.05 ms intervals. The DIC analysis results showed that the strain was non-uniform. For the initial 20 s of light irradiation the composite resin shrank to the level of 50~60% of the final curing shrinkage. Such large shrinkage amount of the composite resin lump affected the tensile stress concentration near the adhesive region between the composite resin and the substrate.

Photoluminescence characteristics of ZnTe single crystal thin films substi-tuted by sulfur (Sulfur에 의하여 치환된 ZnTe 단결정 박막의 광발광 특성)

  • 최용대
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.13 no.6
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    • pp.279-283
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    • 2003
  • In this study, ZnTe : S single crystal thin films substituted by sulfur were grown on GaAs (100) substrates by hot-wall epitaxy. The photoluminescence (PL) characteristics of ZnTe : S single crystal thin films was measured to investigate the effects due to sulfur atoms in the ZnTe layer. The Peak of 2.339 eV identified as the isoelectronic center was observed in low temperature PL spectrum, but PL spectra which the origin had not been well-explained were not observed. Temperature dependence of PL intensities of the light hole free exciton was explained by extrinsic self-trapping. Besides it is reported that the emission lines near absorption edge at room temperature were observed.

MOCVD 공정으로 성장된 ZnO박막의 texture 제어 연구

  • Gang, Hui-Min;Jeong, Jeung-Hyeon;Choe, Heon-Jin;Baek, Yeong-Jun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.49-49
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    • 2011
  • 실리콘 태양전지에 사용되는 ZnO 박막의 특성은 적외선과 가시광선 영역에서 높은 투과도 (>80%)와 낮은 비저항(<10-2) 외에 산란(scattering)에 의한 빛의 광학적 경로(optical path) 증가로 활성층(active layer)에서의 광 흡수도 증가 및 입사광의 재반사를 방지할 수 있는 표면 형상(morphology)의 제어가 중요하다. 일반적으로 우선 배향성(preferred orientation)이 <0002>방향으로 texturing된 ZnO박막보다 <1120>방향으로 texturing된 박막이 더 우수한 광 산란 효과를 보인다. 따라서, 이 논문에서는 유기화학증착공정으로 증착한 ZnO 박막의 texture 형성에 있어 박막 증착 온도 및 원료로 사용하는 DEZ(Diethylzinc)와 H2O의 상대농도 변화에 따른 texture 방향의 변화에 대해 고찰하였다. 반응기내의 압력을 0.67 torr로고정하고 기판온도를 $90^{\circ}C$에서 $170^{\circ}C$까지 $20^{\circ}C$간격으로 증가시키고, $120^{\circ}C$에서 H2O/DEZ의 비를 0.1에서 4까지 변화시켰다. 기판온도가 증가함에 따라 ZnO박막의 texture 방향은 <0002>에서 <1120> 방향으로 변화하였다. 또한 $120^{\circ}C$에서 H2O/DEZ 비가 증가함에 따라 ZnO 박막의 texture 방향은 <0002>에서 <1120> 방향으로 변화하였다. 이에 따른 광투과, 광산란 특성과 전기적 특성의 변화를 조사하였다.

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Optical properties of the $A1_{0.15}$$Ga_{0.85}$N/GaN thin film ($A1_{0.15}$$Ga_{0.85}$N/GaN 박막의 광학적 특성)

  • 정상조;차옥환;서은경;김영실;신현길;조금재;남승재
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.9 no.6
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    • pp.553-557
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    • 1999
  • In order to investigate the optical properties of the $Al_XGa_{1-X}N/GaN$ thin film grown by metalorganic chemical vapor deposition (MOCVD) method, the photoluminescene (PL), photocurrent (PC) and persistent photoconductivity (PPC) measurements were carried out at room temperature. The band gap of the $A1_x$$Ga_{1-x}$N/GaN was determined to 3.70 eV by the PL and PC measurements. The PC measurement on the light illumination from the top of the $A1_x$$Ga_{1-x}$N/GaN thin film provides peaks at 3.70, 3.43, and around 2.2 eV. The PC spectrum by the illumination passing through from the substrate of the sample can be shown at 3.43 eV together with a broad tail band from the GaN band edge to around 2.23 eV. The photocurrent quenching and anomalous PPC decay observed in PPC measurements indicate that metastable electron states are fomed in the band gap of GaN layer to trap electrons which can be tunneled the potential barrier for long recovery time.

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A Study on the Magneto-optical Properties and Application of Diluted Magnetic Semiconductor Cd1-xMnxTe (묽은 자성 반도체 Cd1-xMnxTe의 자기 광학적 특성과 응용성 연구)

  • Hwang, Young-Hun;Um, Young-Ho;Cho, Sung-Lae
    • Journal of the Korean Magnetics Society
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    • v.19 no.5
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    • pp.186-190
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    • 2009
  • We investigated the magneto-optical properties and application of diluted magnetic semiconductors Cd$_{1-x}$Mn$_x$Te crystals with various Mn contents grown using a vertical Bridgman method. This material crystallizes in the zinc-blende structure for values of x < 0.82. The band-gap energy was depended on Mn mole fraction x linearly and increased with decreasing temperature. The Faraday rotation was increased as the photon energy increased near to that of the fundamental band gap and its increased with increasing Mn mole fraction. Optical isolator using the Cd$_{0.62}$Mn$_{0.38}$Te crystal shows that the isolation and insertion loss are 45 dB and 0.35 dB at 650 nm, respectively.

POLYMERIZATION SHRINKAGE OF COMPOSITE RESINS CURED BY VARIABLE LIGHT INTENSITIES (가변 광도 중합에 따른 복합레진의 중합수축에 관한 연구)

  • Lim, Mi-Young;Cho, Kyung-Mo;Hong, Chan-Ui
    • Restorative Dentistry and Endodontics
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    • v.32 no.1
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    • pp.28-36
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    • 2007
  • The purpose of this study was to compare the effect of exponential curing method with conventional curing and soft start curing method on polymerization shrinkage of composite resins. Three brands of composite resins (Synergy Duo Shade, Z250, Filtek Supreme) and three brands of light curing units (Spectrum 800, Elipar Highlight, Elipar Trilight) were used. 40 seconds curing time was given. The shrinkage was measured using linometer for 90 seconds. The effect of time on polymerization shrinkage was analysed by one-way ANOVA and the effect of curing modes and materials on polymerization shrinkage at the time of 90s were analysed by two-way ANOVA. The shrinkage ratios at the time of 20s to 90s were taken and analysed the same way. The results were as follows : 1. All the groups except Supreme shrank almost within 20s Supreme cured by soft start and exponential curing had no further shrinkage after 30s (p < 0.05). 2. Statistical analysis revealed that polymerization shrinkage varied among materials (p = 0.000) and curing modes (p = 0.003). There was no significant interaction between material and curing mode. 3. The groups cured by exponential curing showed the statistically lower polymerization shrinkage at 90s than the groups cured by conventional curing and soft start curing (p < 0.05). 4. The initial shrinkage ratios of soft start and exponential curing were statistically lower than conventional curing (p < 0.05). From this study, the use of low initial light intensities may reduce the polymerization rate and, as a result, reduce the stress of polymerization shrinkage.

EFFECT OF SOFT-START LIGHT CURING ON THE POLYMERIZATION AND THE CONTRACTION STRESS OF COMPOSITE RESIN (완속기시(Soft-start) 광조사 방식이 복합레진의 중합 및 수축응력에 미치는 효과)

  • Wee, You-Min;Oh, You-Hyang;Lee, Nan-Young;Lee, Chang-Seop;Lee, Sang-Ho
    • Journal of the korean academy of Pediatric Dentistry
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    • v.32 no.2
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    • pp.332-343
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    • 2005
  • The purpose of this study was to evaluate the influence of soft-start light curing on contraction stress and hardness of composite resin. Composite resin mold was cured using the one-step continuous curing method with three difference light sources; conventional halogen light curing for 40 seconds at $400\;mw/cm^2$, plasma arc light curing for 6 seconds at $1300\;mW/cm^2$ and LED light curing for 10 seconds at $7The purpose of this study was to evaluate the influence of soft-start light curing on contraction stress and hardness of composite resin. Composite resin mold was cured using the one-step continuous curing method with three difference light sources; conventional halogen light curing for 40 seconds at . For the soft-start curing method ; 2 seconds light exposure at $650\;mW/cm^2$ followed by 3 seconds at $1300\;mW/cm^2$ and exponential increase with 5 seconds followed by 10 seconds at $700\;mW/cm^2$ were used. Contraction stress was measured using strain gauge method and Vickers hardness was measured 24 hours after polymerization at the top and bottom of specimens. Resin-acrylic interfaces were observed using a scanning electron microscope(SEM). The results of present study can be summarized as follows: 1. Contraction stresses at 10 min after polymerization were significantly reduced with the soft-start curing both in plasma and LED light sources(P<0.05). 2. Plasma light curing with soft-start resulted in not only the lowest contraction stress, but also the lowest hardness(P<0.05) 3. LED light curing with soft-start showed lower contraction stress than the one-step continuous halogen and LED light curing(P<0.05). 4. Microhardness of specimens cured by LED light with soft-start was equivalent to that of cured by the one-step continuous halogen and LED light(P>0.05). 5. Curing by LED light with soft-start and conventional halogen light resulted in better marginal sealing than plasma light and one-step LED light curing.

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Photoluminescence from silicon nanocrystals in silicon ion implanted SiO2 layers (실리콘 이온주입 SiO2층의 나노결정으로 부터의 광루미네센스)

  • Kim, Kwang-Hee;Oh, Hang-Seok;Jang, Tae-Su;Kwon, Young-Kyu;Lee, Yong-Hyun
    • Journal of Sensor Science and Technology
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    • v.11 no.3
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    • pp.183-190
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    • 2002
  • Photoluminescence(PL) properties of $Si^+$-implanted $SiO_2$ film, which was thermally grown on c-Si substrate, is reported. We have compared room temperature photoluminescence (PL) spectra of the samples which was made in several kinds of implantation, subsequent annealing and $SiO_2$ film thickness. XRD data was correlated with the PL spectra. Silicon nanocrystals in $SiO_2$ film is considered as the origin of the photoluminescence. PL spectra was investigated after wet etching of the $SiO_2$ film by using BOE (Buffered Oxide Etchant) at every one minute. PL peak wavelength was varied as the etching is proceeded. These results indicate that the quantity and the distribution of dominant size of Si nanocrystals in $SiO_2$ film seem to have a direct effect on PL spectrum.

나노 임프린팅 공정을 이용한 Ag Nano Rod 제조 및 박막 태양전지 적용

  • Kim, Min-Jin;Sin, Jang-Gyu;Kim, Yang-Du;Go, Bit-Na;Kim, Ga-Hyeon;Lee, Jeong-Cheol;Kim, Dong-Seok
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.414-414
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    • 2014
  • 박막 태양전지의 광흡수를 증가시키기 위한 방법으로 나노 사이즈의 구조체를 이용하는 방법들이 주목받고 있다. 나노 구조체로 인한 광 산란 효과는 광 흡수층에서 빛의 흡수를 높여 태양전지의 변환효율을 높일 수 있다. 3차원 구조체를 제작하는 기존의 방법들은 대면적 기판에 적용이 어렵고, 비용적 측면 등의 문제점들이 있다. 본 연구에서는 대면적화가 가능한 나노 임프린트 리소그래피 방법을 이용하여 Ag nano rod 패턴을 제작하였다. 임프린트 공정 중 UV 조사시간, 가해지는 하중, 기판온도 등의 변수들과, 건식 이온 식각 시 변수들을 조절하여 최적화된 3차원 rod 패턴을 형성할 수 있었다. 그림 1은 형성된 Ag rod 패턴의 SEM 측정 사진이다. 전극 폭 300 nm, 간격 300 nm로 제조된 rod는 Ag의 두께를 조절함으로써 전기, 광학적 특성을 조절할 수 있었다. 3차원 Ag nano rod를 박막 태양전지의 전, 후면 전극으로 사용하여 태양전지의 특성변화를 분석하였다.

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