• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2008년도 추계학술대회 논문집 Vol.21
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• pp.450-451
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• 2008

비정질 실리콘 태양전지는 n-i-p형 구조가 일반적이며, 각 층의 두께와 도핑농도가 태양전지의 효율을 결정하는 중요한 요인이다. 최대의 효율을 얻을 수 있는 태양전지 설계를 위해 AFORS HET 시뮬레이션을 통하여 n층의 두께와 도핑농도, 그리고 p층의 도핑농도롤 변화시켰다. 최적화 결과, a-Si:H(n) 층의 두께 1nm, a-Si:H(n)층의 도핑농도 $2\times10^{20}cm^{-3}$, a-Si:H(p+)층의 도핑농도 $1\times10^{19}cm^{-3}$에서 $V_{oc}$=679.5mV, $J_{sc}$=39.02mA/$cm^2$, FF=83.71%, Efficiency=22.21%의 고효율을 얻을 수 있다. 본 연구를 통하여 실제의 높은 효율을 갖는 태양전지 설계와 제조 시에 이용할 수 있을 것이다.

• 한국재료학회지
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• 제27권2호
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• pp.107-112
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• 2017

The BCBJ (Back Contact and Back Junction) or back-lit solar cell design eliminates shading loss by placing the pn junction and metal electrode contacts all on one side that faces away from the sun. However, as the electron-hole generation sites now are located very far from the pn junction, loss by minority-carrier recombination can be a significant issue. Utilizing Medici, a 2-dimensional semiconductor device simulation tool, the interdependency between the substrate thickness and the minority-carrier recombination lifetime was studied in terms of how these factors affect the solar cell power output. Qualitatively speaking, the results indicate that a very high quality substrate with a long recombination lifetime is needed to maintain the maximum power generation. The quantitative value of the recombination lifetime of minority-carriers, i.e., electrons in p-type substrates, required in the BCBJ cell is about one order of magnitude longer than that in the front-lit cell, i.e., $5{\times}10^{-4}sec$ vs. $5{\times}10^{-5}sec$. Regardless of substrate thickness up to $150{\mu}m$, the power output in the BCBJ cell stays at nearly the maximum value of about $1.8{\times}10^{-2}W{\cdot}cm^{-2}$, or $18mW{\cdot}cm^{-2}$, as long as the recombination lifetime is $5{\times}10^{-4}s$ or longer. The output power, however, declines steeply to as low as $10mW{\cdot}cm^{-2}$ when the recombination lifetime becomes significantly shorter than $5{\times}10^{-4}sec$. Substrate thinning is found to be not as effective as in the front-lit case in stemming the decline in the output power. In view of these results, for BCBJ applications, the substrate needs to be only mono-crystalline Si of very high quality. This bars the use of poly-crystalline Si, which is gaining wider acceptance in standard front-lit solar cells.

• Archives of Plastic Surgery
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• 제32권3호
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• pp.357-362
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• 2005

The aim of this study is to elucidate the effect of keratinase on epidermis of rat skin. Twenty-five male Sprague-Dolly rats were used. The hair on the back were removed and $2{\times}2cm$ area was marked. The rats were divided five groups; 1) Control group(Co), 2) Cleansing gel group(Cl), 3) Cleansing gel+keratinase group, 4) Exfoliant gel group(Ex), and 5) Exfoliant gel+ keratinase group(Ex+K). The solutions were applied to the back area twice a day for five days. On fifth day, the skins were harvested, fixed and prepared for histologic sections. The thickness of keratin layer, living epidermis, dermis, and cell layer number of living epidermis were measured. In the group containing keratinase(Cl+K, Ex+K), the thickness of keratin layer and living layer were thinner than other groups. However, there were no significant differences of the cell layer number of living epidermis and thickness of the dermis among the five groups. We think the keratinase may have the effect thinning the keratin layer as well as the thickness of living epidermis, without effecting the living cell and dermal component. The keratinase containing soap may be of benefit to remove the excess keratin layers in human.

• 대한안전경영과학회지
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• 제17권4호
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• pp.397-401
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• 2015

In this study, analysed the characteristics of power drop and surface damage in solar cell through high temperature and humidity test in the 3 case of EVA(ethylene vinyl acetate) and 2 case ribbon thickness. The solar cells were tested during the 500hr in $85^{\circ}C$ temperature and 85% relative humidity conditions, that excerpted standard of PV Module(KS C IEC-61215). Through the EL(Electroluminescence) shots, specimen's surface have partialy damaged. Before and after high humidity and high temperature test, ribbon thickness $200{\mu}m$ EVA1 case power drop rate was 8.463%, EVA2 case was 6.667%, EVA3 case was 6.373%. In the ribbon thickness $250{\mu}m$ EVA1 case power drop rate was 6.521%, EVA2 case was 8.517%, EVA3 case was 6.019%. EVA3 case was the lowest power and FF(fill factor) drop rate at the 2 case of ribbon thickness, because EVA3 is laerger than EVA1 and EVA2 in thickness, elongation and tensile strength.

• 한국세라믹학회지
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• 제34권3호
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• pp.225-232
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• 1997

고율 방전용 Li/SOCl2전지의 성능은 카본 양극에 의해 크게 영향을 받는다. 전지가 방전되는 동안 SOCl2의 환원은 다공성 카본 양극에서 일어나고 기공내에 방전반응 생성물-주로 LiCl-이 석출된다. 이러한 현상으로 양극 표면이 부동화되어 전지의 성능이 제한된다. 양극이 성능을 향상시키기 위해 양극이 표면밀도와 두께를 각각 변화시켜 양극 반쪽셀 정전류 방전실험(50mA/$\textrm{cm}^2$)을 행하였다. 실험 결과 0.04g/$\textrm{cm}^2$, 두께 1.4mm의 양극이 가장 좋은 특성을 보였다. 표면 밀도가 0.04 g/$\textrm{cm}^2$로 일정하고 두께가 0.8mm, 1.4mm의 양극에서 분극현상은 두께가 두꺼운 1.4mm양극에서 감소하였으며 방전경과시간과 방전용량(Ah/$\textrm{cm}^2$)이 증가하였다. 두 양극에 대한 기공률 측정 결과 두께 1.4mm양극이 두께 0.8mm양극보다 전체 기공부피가 크고 전지성능과 연관되는 mesopore(0.05 $\mu$m~0.5$\mu$m)와 macropore(>0.5$\mu$m)부피가 더 증가하였다. 방전 후 카본 양극의 표면분석 결과 등방결정과 판상구조 집합체 형태의 LiCl과 소량의 S를 확인하였다.

• 한국전기전자재료학회논문지
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• 제11권5호
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• pp.384-393
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• 1998

A mixed powder of electrolyte and matrix support materials with a proper proportion was used for the fabrication of an electrolyte matrix sheet. The purpose of this study is to reduce the large change in MCFC cell thickness occurring in the initial start-up period when separate sheets of electrolyte and support are used. A focus was put on how small the carbonate particles could be made. The particle size of the carbonate powder was controlled by ball milling and the distribution was measured using a particle size analyser. The thickness change was reduced to 20% by this approach, which could be compared to 27% observed in a conventional cell. The thickness changes of electrolyte matrix have linear relation sizes of carbonate powders.

• 대한수의학회지
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• 제28권2호
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• pp.221-226
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• 1988

Normal swine brains at 1 to 70 days after birth were used to investigate the presence and morphology of the subependymal layer (SL) in the ventricle walls. The brain samples were taken from 27 pigs of 4 swine breeds. The results were summarized as follows: 1. SLs were observed on the walls of the lateral ventricle (LV) but none were observed on the walls of the 3th and 4th ventricles. 2. SLs of the LV walls were composed of mainly 3-to 10-cell layers in thickness. The thinest region of SLs was composed of only 1-to 2-cell thick on the dorsal and ventral walls, and the thickest region was composed of 250-to 300-cell thick on extension region of the SLs into the angle between the corpus callosum and caudate nucleus. 3. Of the LV parts observed, the SL thickness were 25-to 45-cell thick on the anterior horn, 3-to 10-cell thick on the body, 100-to 220-cell thick on the angle region between the corpus callosum and caudate nucleus, and 3-to 5-cell thick the superior walls of the posterior horn. Also the SL thickness was more thick on the anterior region than those on the posterior region. 4. SLs may be classified as three types by the cell distribution; one type of them is closely arranged cell region with the distinctive lateral margin from the periventricular white matter, the other type is loosely arranged cell region with the undistinctive lateral margin, and another type is two-subdivided region as the loosely and closely arranged cell layers in a layer. 5. SLs were extensively thick in young age but gradually decreased in size and cell number with age after 20-day age. SL layers were composed of mainly oligodendrocytes, astrocytes and immature cells of them. Morphological differences of SL in different breeds of pigs were not observed.

• 한국진공학회지
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• 제11권3호
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• pp.166-170
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• 2002

$BaTiO_3$(BTO)/$SrTiO_3$(STO) 산화물 인공 초격자가 MgO(100) 단결정 기판위에 Pulsed laser deposition(PLD)법으로 증착되었다. 다층구조에서 BTO/STO 층의 적층 주기는 $BTO_{1\;unit\; cell}/STO_{1\;unit\; cell}$에서 $BTO_{125\;unit\; cell}/STO_{125 \;unit \;cell}$ 두께로 변화시켰고 초격자 전체 두께는 100 m으로 고정시켰다. X-ray 회절 결과는 다양한 주기의 BTO/STO 산화물 박막에서 초격자의 특성을 보였고 투과형 전자 현미경을 통해서 BTO와 STO의 두 층간의 계면에서 상호확산이 일어나지 않고 초격자가 잘 성장된 것을 확인하였다. 초격자의 유전율은 임계 두께 내에서 적층주기가 감소함에 따라 증가하였다. 이러한 초격자의 유전율은 낮은 주기 즉 $BTO_{2\;unit\; cell}/STO_{2\;unit\; cell}$ 주기에서 1230으로 높게 나왔으며 이러한 원인은 격자 변형(c/a ratio)에 기여된 것으로 분석되었다.

• 전기화학회지
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• 제11권1호
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• pp.1-5
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• 2008

A Pt-layer was deposited on the anode side of a Nafion membrane via a sputtering method in order to reduce methanol crossover in a direct methanol fuel cell (DMFC). The methanol permeation and the proton conductivity through the modified membranes were investigated. The performances of the direct methanol fuel cell were also tested using single cells with a Nafion membrane and the modified membranes. The Pt-layers on the membrane blocked both methanol crossover and proton transport through the membranes. Methanol permeability and proton conductivity decreased with an increase of the platinum layer thickness. At methanol concentration of 2 M, the DMFC employing the modified membrane with a platinum layer of 66 nm-thickness showed similar performance to that of a DMFC with a bare Nafion membrane in spite of the lower proton conductivity of the former. The maximum power density of the cell using the modified membrane with a platinum layer of 66 nm-thickness increased slightly while that of the cell with the bare membrane decreased abruptly when a methanol solution of 6M was supplied.

• 한국태양에너지학회 논문집
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• 제39권3호
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• pp.9-17
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• 2019

Laser cutting cell of solar cells can achieve high voltage and efficiency through more array than conventional 6 inch cell compared to same area. In this study, we fabricated c-Si cutting cell with various lasers and laser conditions such as power, speed, and number of times. In the case of picosecond laser, excellent surface characteristics were obtained due to small surface defects and low thermal damage at the output of 20W and the speed of 100 mm/s. However, it is not possible to fabricate a cutting cell having good characteristics due to nonuniform cutting inside the wafer when the processing for forming a cutting cell is not sufficiently performed. For nanosecond lasers, the best wafer characteristics were obtained for fabrication of excellent cutting cells at a frequency of 500 kHz and a laser speed of 100 mm/s. However, the nanosecond laser has not been processed sufficiently in the condition of a number of times. As a result, it was confirmed that the wafer thickness was cut by $63{\mu}m$ of the cell thickness of $170{\mu}m$ in the condition of five times of laser process. It was found that more than 30% of the wafer thickness had to be processed to fabricate the cutting cell. After cutting the 6-inch cell having the voltage of 0.65 V, we obtained the voltage of about 0.63 V.