• Title/Summary/Keyword: Back-contact layer

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Construction of the Intelligence Stress Predictor for Compression Strength Evaluation (압축강도 평가를 위한 지능형 응력예측기 구축)

  • 박원규;우영환;이종구;윤인식
    • Transactions of the Korean Society of Machine Tool Engineers
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    • v.10 no.6
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    • pp.95-101
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    • 2001
  • This work is concerned with construction of the intelligence stress predictor far compression strength evaluation using neural network-ultrasonic waves. The contact pressure in jointed plates was measured by using ultrasonic technique. Neural network is used to evaluate and predict contact pressure from the results of the calibration curves. The organized neural system was leaned with the accuracy of 99%, as a result of learning the ultrasonic echo ratio to the contact pressure measurement between SM45C and STS410 materials. And it could be evaluated and predicted with the accuracy of 90% in the evaluation of ultrasonic echo ratio difference in the same surface roughness and contact pressure, and 85% in the prediction of virtual ultrasonic echo ratio. Thus the proposed stress predictor is very useful for the evaluation and prediction of the contact pressure between SM45C and STS410 materials.

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A Study on the CIGS cells with Na-doped Mo back contact (Na이 첨가된 Mo 전극을 이용한 CIGS 박막 태양전지 연구)

  • Yun, Jae-Ho;Kim, Ki-Hwan;Kim, Min-Sik;Ahn, Byung-Tae;Ahn, Se-Jin;Lee, Jeong-Chul;Yoon, Kyung-Hoon
    • 한국신재생에너지학회:학술대회논문집
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    • 2006.06a
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    • pp.218-221
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    • 2006
  • The photovoltaic properties of CIES cells on alumina substrate were improved by using the Na-doped Mo as theabotom layer of hilo back contact. Na was supplied to the CIGS bulk region from alumina/Na-doped Mo/Mo/alumina? structure, as same assimilar to the Na diffusion from soda-lime glass. The content diffusion of Na from Na-doped bfo was smaller more controlled than that from SLG. These Our results indicate that Na-doped bfo act as Na source material and contents of Na amount can be controlled without the use of an alkali barrier layer. The best CIGS solar cell with conversion efficiency of 13.34%, $J_{sc}=34.62mA/cm^2,\;V_{oc}=0.58V$ and FF=66% for an active area of $0.45cm^2$ on the alumina substrate was obtained in the condition of for 100nm Na-doped Mo/1000nm Mo.

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Local-Back Contact Solar Cell adapted Laser ablation on ONO structure passivation layer

  • Gong, Dae-Yeong;Yu, Gyeong-Yeol;Lee, Jun-Sin
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.08a
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    • pp.325-325
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    • 2010
  • 최근 결정질 실리콘 태양전지 분야에서는 태양전지의 Voc와 Isc의 증가를 통한 효율 향상을 목적으로 후면 passivation에 대한 연구가 활발하게 진행되고 있다. Local-Back Contact은 최적화된 후면 passivation 박막을 이용한 태양전지 제조방법이다. 고효율 태양전지 개발을 위해 최적의 laser 가공 조건이 확립되어야 한다. 본 연구에서는 고효율의 LBC 태양전지 개발을 위해 ONO 구조의 후면 passivation 박막에 laser ablation 조건을 가변하여 LBC 태양전지를 제작하고 그 특성을 분석하였다. 본 연구에 사용된 laser는 355nm 파장을 갖는 UV laser를 사용하였다. laser 파워는 5W, 주파수는 30kHz로 하였을 때 폭 20um, 깊이 5um의 홀을 형성시킬 수 있었다. 후면 접촉 면적의 영향을 확인하기 위하여 laser ablation 간격을 300um, 500um, 700um으로 가변하여 공정을 진행하였다. 태양전지 제조 결과 spacing 300um일 경우 효율이 높게 측정되었으며, laser ablation의 데미지를 줄이기 위한 FGA 처리시 웨이퍼 표면의 데미지를 줄여 carrier lifetime 향상에 기여하는 것을 확인할 수 있었다. 본 연구의 결과를 이용하여 향후 후면 passivation 극대화 및 접촉면적 가변을 통한 고효율 LBC 태양전지 개발이 가능할 것으로 판단된다.

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An Analysis on rear contact for crystalline silicon solar cell (결정질 실리콘 태양전지에 적용하기 위한 후면전극 형성에 관한 연구)

  • Kwon, Hyukyong;Lee, Jaedoo;Kim, Minjung;Lee, Soohong
    • 한국신재생에너지학회:학술대회논문집
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    • 2010.06a
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    • pp.91.1-91.1
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    • 2010
  • There are some methods for increasing efficiency of crystalline silicon solar cells. Among them, It is important to reduce the recombination loss of surface for high efficiency. In order to reduce recombination loss is a way to use the BSF(Back Surface Field). The BSF on the back of the p-type wafer forms a p+layer. so, it is prevented to act electrons of the p-area for the rear recombination. As a result, the leakage current is reduced and the rear-contact has a good Ohmic contact. therefore, open-circuit-voltage and Fill factor(FF) of solar cells are increased. This paper investigates the formation of rear contact process comparing Aluminum-paste(Al-paste) with Aluminum-Metal(99.9%). It is shown that the Aluminum-Metal provides high conductivity and low contact resistance of $21.35m{\Omega}cm$ using the Vacuum evaporation process but, it is difficult to apply the standard industrial process because high Vacuum is needed and it costs a tremendous amount more than Al-paste. On the other hand, using the Al-paste process by screen printing is simple for formation of metal contact and it is possible to produce the standard industrial process. however, it is lower than Aluminum-Metal(99.9) of conductivity because of including mass glass frit. In this study, contact resistances were measured by 4-point prove. each of contact resistances is $21.35m{\Omega}cm$ of Aluminum-Metal and $0.69m{\Omega}cm$ of Al-paste. and then rear contact have been analyzed by Scanning Electron Microscopy(SEM).

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Formation of Ohmic Contact in P-Type CdTe Using Cu2 Te Electrode and Its Effect on the Photovoltaic Properties of CdTe Solar Cells (Cu2Te 배면 전극을 이용한 p-type CdTe 태양전지의 ohmic contact 형성 및 CdTe 태양전지의 광전압 특성)

  • Kim, Ki-Hwan;Yun, Jae-Ho;Lee, Doo-Youl;Ahn, Byung-Tae
    • Korean Journal of Materials Research
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    • v.12 no.12
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    • pp.918-923
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    • 2002
  • In this work, CdTe films were deposited on CdS/ITO/glass substrate by a close spaced sublimation (CSS) method. A $Cu_2$Te layer was deposited on the CdTe film by evaporating $Cu_2$Te powder. Then the samples were annealed for p+ ohmic contact. TEM and XRD analysis showed that $CdTe/Cu_2$Te interface exhibited different forms with various annealing temperature. A good p+ ohmic contact was achieved when the annealing temperature was between $180^{\circ}C$ to $200^{\circ}C$. Best cell efficiency of 12.34% was obtained when post annealing temperature was $200^{\circ}C$ for 5 min. Thermal stress test of the CdS/CdTe cells with carbon back contact showed that the $Cu_2$Te contact was stable at $50^{\circ}C$ in $N_2$ and was slowly degraded at $100^{\circ}C$ in $N_2$. In comparison to the conventional carbon contact, the $Cu_2$Te contact showed a better thermal stability.

Local Back Contact Formed by Screen Printing and Atomic Layer Deposited Al2O3 for Silicon Solar Cell

  • Jo, Yeong-Jun;Jang, Hyo-Sik
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.687-687
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    • 2013
  • In rearpoint contact solar cell and the PERC (passivated emitter rear contact) type cell, surfaces were passivated by SiO2 or Al2O3 to increase solar cell efficiency. Therefore, we have investigated the effect of surface passivation for crystalline silicon solarcell using mass-production atomic layer deposited (ALD) Al2O3. The patttern which consists of cylinders with 100um diameter and 5um height was formed by PR patterning on Si (100) substrate and then Al2O3 of about 10nm and 20nm thickness was deposited by ALD. The pattern in 10 nm Al2O3 film was removed by dipping in aceton solution for about 10 min but the pattern in 20 nm Al2O3 film was not. The influences of process temperature and heat treatment were investigated using microwave photoconductance decay (PCD) and Quasi-Steady-State photoconductance (QSSPC). The solar cell process used in this work combines the advantage of using the applicability of a selective deposition associated with a ALD passivation and the use of low-cost screen print for the contacts formation.

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Optimization of ZnO:Al properties for $CuInSe_2$ superstrate thin film solar cell

  • Lee, Eun-U;Park, Sun-Yong;Lee, Sang-Hwan;Kim, U-Nam;Jeong, U-Jin;Jeon, Chan-Uk
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2010.05a
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    • pp.36.1-36.1
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    • 2010
  • While the substrate-type solar cells with Cu(In,Ga)Se2 absorbers yield conversion efficiencies of up 20%[1], the highest published efficiency of Cu(In,Ga)Se2 superstrate solar cell is only 12.8% [2]. The commerciallized Cu(In,Ga)Se2 solar cells are made in the substrate configuration having the stacking sequence of substrate (soda lime glass)/back contact (molybdenum)/absorber layer (Cu(In,Ga)Se2)/buffer layer (cadmium sulfide)/window layer (transparent conductive oxide)/anti reflection layer (MgF2) /grid contact. Thus, it is not possible to illuminate the substrate-type cell through the glass substrate. Rather, it is necessary to illuminate from the opposite side which requires an elaborate transparent encapsulation. In contrast to that, the configuration of superstrate solar cell allows the illumination through the glass substrate. This saves the expensive transparent encapsulation. Usually, the high quality Cu(In,Ga)Se2 absorber requires a high deposition temperature over 550C. Therefore, the front contact should be thermally stable in the temperature range to realize a successful superstrate-type solar cell. In this study, it was tried to make a decent superstrate-type solar cell with the thermally stable ZnO:Al layer obtained by adjusting its deposition parameters in magnetron sputtering process. The effect of deposition condition of the layer on the cell performance will be discussed together with hall measurement results and current-voltage characteristics of the cells.

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Fabrication of Flexible CIGS thin film solar cells using STS430 substrate (STS430 기판을 이용한 Flexible CIGS 박막 태양전지 제조)

  • Jung, Seung-Chul;Ahn, Se-Jin;Yun, Jae-Ho;Yoon, Kyung-Hoon
    • 한국신재생에너지학회:학술대회논문집
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    • 2008.05a
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    • pp.436-437
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    • 2008
  • Flexible CIGS thin film solar cell was fabricated using STS430 plate as a flexible substrate in this work. A diffusion barrier layer of $SiO_2$ thin film was deposited on STS430 substrate by PECVD followed by deposition of double layered Mo back contact. After depositing CIGS absorber layer by co-evaporation, CdS buffer layer by chemical bath deposition, ZnO window layer by RF sputtering and Al electrode by thermal evaporation, the solar cell fabrication processes were completed and its performance was evaluated. Corresponding solar cell showed an conversion efficiency of 8.35 % with $V_{OC}$ of 0.52 V, $J_{SC}$ of 26.06 mA/$cm^2$ and FF of 0.61.

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Effects of Mixing Condition and Filtration Velocity on Turbidity Removal in a Contact Roughing Filter (접촉여과방식 거친여과지에서 혼화조건과 여과속도가 고탁도 제거에 미치는 영향)

  • Park, Noh-Back;Park, Sang-Min;Hong, Jin-Ah;Jun, Hang-Bae
    • Journal of Korean Society of Water and Wastewater
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    • v.21 no.3
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    • pp.359-366
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    • 2007
  • Slow sand filtrations have been widely used for water treatment in small communities, however their capacity is often limited by high turbidity in the raw water. For this reason, several pre-treatment facilities were required for a slow sand filter. Turbidity removal from the highly turbid raw water was investigated in roughing filters as a pre-treatment process. The roughing filters followed by rapid mixing tank were operated in the form of a contact filtration. In several jar tests, the predetermined optimum aluminium sulfate (alum) doses for turbid water of 30 and 120NTU were 30 and 50mg/L, respectively. At the optimum alum dose, physically optimum parameters including G value of $220sec^{-1}$ and rapid mixing time of 3 minutes were applied to the contact filtration system. Without addition of alum, the filtrate turbidity from the roughing filters, packed respectively with different media such as sand, porous diatomite ball and gravel, was in the range of 5~30NTU at filtration velocities of 30 and 50m/day. However, the application of a contact filtration to roughing filters showed stably lower filtrate turbidity below 1.0NTU at filtration velocity of 30 m/day. Although the filtration velocity increased to 50m/day, filtrate turbidity was still below 1.0NTU in both single and double layer roughing filters. At influent turbidity of 120NTU, the filtrate turbidity was over 5 NTU in the triple layer roughing filter, which shortened the filter run time. The flocs larger than $10{\mu}m$, formed in the rapid mixing tank, were almost captured through the roughing filter bed, while the almost flocs smaller than $10{\mu}m$ remained in filtrate.

Analysis of Subwavelength Metal Hole Array Structure for the Enhancement of Quantum Dot Infrared Photodetectors

  • Ha, Jae-Du;Hwang, Jeong-U;Gang, Sang-U;No, Sam-Gyu;Lee, Sang-Jun;Kim, Jong-Su;Krishna, Sanjay;Urbas, Augustine;Ku, Zahyun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.02a
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    • pp.334-334
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    • 2013
  • In the past decade, the infrared detectors based on intersubband transition in quantum dots (QDs) have attracted much attention due to lower dark currents and increased lifetimes, which are in turn due a three-dimensional confinement and a reduction of scattering, respectively. In parallel, focal plane array development for infrared imaging has proceeded from the first to third generations (linear arrays, 2D arrays for staring systems, and large format with enhanced capabilities, respectively). For a step further towards the next generation of FPAs, it is envisioned that a two-dimensional metal hole array (2D-MHA) structures will improve the FPA structure by enhancing the coupling to photodetectors via local field engineering, and will enable wavelength filtering. In regard to the improved performance at certain wavelengths, it is worth pointing out the structural difference between previous 2D-MHA integrated front-illuminated single pixel devices and back-illuminated devices. Apart from the pixel linear dimension, it is a distinct difference that there is a metal cladding (composed of a number of metals for ohmic contact and the read-out integrated circuit hybridization) in the FPA between the heavily doped gallium arsenide used as the contact layer and the ROIC; on the contrary, the front-illuminated single pixel device consists of two heavily doped contact layers separated by the QD-absorber on a semi-infinite GaAs substrate. This paper is focused on analyzing the impact of a two dimensional metal hole array structure integrated to the back-illuminated quantum dots-in-a-well (DWELL) infrared photodetectors. The metal hole array consisting of subwavelength-circular holes penetrating gold layer (2DAu-CHA) provides the enhanced responsivity of DWELL infrared photodetector at certain wavelengths. The performance of 2D-Au-CHA is investigated by calculating the absorption of active layer in the DWELL structure using a finite integration technique. Simulation results show the enhanced electric fields (thereby increasing the absorption in the active layer) resulting from a surface plasmon, a guided mode, and Fabry-Perot resonances. Simulation method accomplished in this paper provides a generalized approach to optimize the design of any type of couplers integrated to infrared photodetectors.

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