• 제목/요약/키워드: Thin-Film Solar Cell

검색결과 622건 처리시간 0.028초

실리콘 박막 태양전지용 터널접합 특성연구 (Study of the tunnel recombination junction performance in thin film tandem solar cell)

  • 장지훈;이정철;송진수;윤경훈
    • 한국신재생에너지학회:학술대회논문집
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    • 한국신재생에너지학회 2007년도 추계학술대회 논문집
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    • pp.278-280
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    • 2007
  • a-Si:H/${\mu}$c-Si:H 적층형 태양전지의 효율향상을 위해 상부전지와 하부전지간의 접합특성은 매우 중요하다. 본 연구에서는, 접합특성을 향상하기 위하여 아몰퍼스 보다 전도도가 높은 마이크로화된 n층 또는 ZnO:Al을 중간층으로 삽입한 태양전지를 제조하였으며, 그 특성을 전기적, 광학적 방법으로 분석하였다. 전기적 특성에서, 상부전지 n층에 아몰퍼스를 적용한 태양전지의 경우, 상부전지와 하부전지 간의 직렬저항이 $500{\Omega}-cm^2$ 이상으로 높게 측정되었고, 이에 따라 AM 1.5 상태의 I-V 특성에서 비틀림 현상이 발생하여 곡선인자(Fill Factor : FF)가 낮게 측정되었다. 이에 반하여, 상부전지 n층에 마이크로층을 적용하거나, ZnO:Al 중간층을 삽입한 시편의 경우, 상부전지와 하부전지간의 직렬저항이 $1{\Omega}-cm^2$ 이하로 감소하였으며, 이와 같은 계면간의 접합특성 향상으로 I-V특성에서 비틀림 현상이 사라지고, FF가 70% 까지 증가하였다. 또한, 마이크로층과 ZnO:Al 중간층을 동시에 적용한 태양전지의 경우, FF가 75%까지 가장 높게 증가하였다. 광학적 특성의 경우, 같은 두께의 아몰퍼스 n층에 비하여 마이크로 n층이 투과도는 더 높게, 반사도는 낮게 측정되었으며, 이는 하부전지의 단락전류 (Short circuit current : Jsc)를 높여줄 것으로 판단된다.

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굽힘 시험에 의한 플렉시블 CZTS 태양전지의 I-V 특성 변화에 관한 연구 (Change of I-V Properties of Flexible CZTS Solar Cell Through Mechanical Bending Test)

  • 김성준;김제하
    • 한국융합학회논문지
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    • 제13권3호
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    • pp.197-202
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    • 2022
  • CZTS 태양전지는 Cu, Zn, Sn, Se, S으로 구성된 흡수층을 사용하는 박막 태양전지로, In, Ga이 사용되는 CIGS 태양전지보다 저렴하며 Pb, Cd이 사용된 페로브스카이트, CdTe 태양전지보다 친환경적이다. 본 연구에서 우리는 유연기판인 Mo foil 위에 제작된 유연 CZTS 태양전지를 지정된 곡률만큼 휘게 하는 bending test를 진행하였다. 태양전지에 압축응력이 가해지는 inner benidng과 인장응력이 가해지는 outer bending의 방향에서 실험은 진행되었으며, 50 mmR의 곡률 반경으로 진행된 1,000 회의 굽힘 횟수 동안 태양전지의 효율은 최고 12.7%까지 감소하였으며, 두 방향 모두에서 효율 감소의 가장 큰 원인은 병렬저항의 큰 감소로 나타났다.

플라즈마 화학증착법으로 제작한 미세결정질 실리콘 박막 특성에 관한 연구 (A study on Characteristics of Microcrystalline Silicon Films Fabricated by PECVD Method)

  • 이종하;이병욱;이호년;김창교
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2008년도 춘계학술대회 및 기술 세미나 논문집 디스플레이 광소자
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    • pp.57-58
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    • 2008
  • Microcrystalline (${\mu}c$) silicon thin films were prepared on glass by plasma-enhanced-chemical-vapor-deposition (PECVD) at various substrate temperature, and dilution ratio of $H_2$ with $SiH_4$. The structural and optical properties of. the ${\mu}c-Si$ thin films were investigated using XRD and UV-VIS spectrophotometer. The ${\mu}c-Si$ thin film with 42 nm grain size was grown at optimal condition of 2.5 Torr, spacing between electrodes of 3cm, deposition time of 3000s, RF power of 200W, substrate temperature of $350^{\circ}C$, $SiH_4$ ($20%SiH_4$+80%He) of 50sccm, and $H_2$ of 100sccm.

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AZO 박막의 전기전도특성 및 필름형 염료 태양전지의 광전 변환 특성 (Electrical Conduction Mechanism of AZO Thin Film and Photo-Electric Conversion Efficiency of Film-Typed Dye Sensitized Solar Cell)

  • 곽동주
    • 조명전기설비학회논문지
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    • 제24권4호
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    • pp.66-72
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    • 2010
  • 본 연구에서는 플렉시블 염료감응 태양전지(F-DSC)의 투명전도막으로서의 적용 가능성을 평가하기 위하여 PET 기판위에 AZO 박막을 증착하였다. 또한 ITO와 AZO 박막을 이용하여 동일한 조건하에서 F-DSC를 제작하여 광변환효율을 조사하였다. AZO의 경우 체적저항율 및 증착율은 220[W]의 전력조건하에서 각각 $1.8{\times}10^{-3}[{\Omega}{\cdot}cm]$와 25.5[nm/min] 정도였으며, 광투과율은 약 87[%]였다. AZO 박막의 전기전도 메카니즘의 방전전력 의존성은 XPS 분석결과 방전전력이 증가함에 따라 O1s/Zn2p의 성분비가 증가하여 산소성분에 의한 도너 제공에 크게 영향을 받는 것으로 나타났다. 한편, AZO 투명전도막으로 제작된 F-DSC의 변환효율은 약 2.79[%] 정도였으며, 이는 상용 ITO의 2.94[%]에 거의 필적되는 값으로 AZO의 F-DSC에의 응용 가능성이 충분함을 알 수 있었다.

비정질 p-SiC/i-SiC/i-Si/n-Si 박막 태양전지에서 i-SiC 완충층의 역할 (Roles of i-SiC Buffer Layer in Amorphous p-SiC/i-SiC/i-Si/n-Si Thin Film Solar Cells)

  • 김현철;신혁재;이재신
    • 한국재료학회지
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    • 제9권12호
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    • pp.1155-1159
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    • 1999
  • 플라즈마 화학증착 (PECVD) 장비를 이용하여 $SnO_2$ 투명전도막이 피막된 유리기판 위에 p-SiC/i-Si/n-Si 이종접합 태양전지를 제작하였다. p-SiC 층의 증착중에 기체조성 x=$CH_4/\;(SiH_4+CH_4)$의 변화에 대한 태양전지의 광기전 특성을 관찰하였다. 기체조성(x)이 0~0.4의 범위에서 p-SiC 창층의 광학적 밴드갭의 증가로 인하여 태양전지의 효율은 증가하였으나, 그 이상의 기체조성에서는 p-SiC/i-Si 계면에서의 조성불일치가 증가하여 태양전지의 효율이 감소하였다. 이러한 계면문제는 p-SiC 층과 i-Si 계면에서의 조성불일치가 증가하여 태양전지의 효율이 감소하였다. 이러한 계면문제는 p-SiC 층과 I-Si 층 사이에 I-SiC 완충층을 삽입함으로써 크게 감소하였다. 그 결과 유효면적이 $1cm^2$인 glass/$SnO_2$/p-SiC/i-SiC/i-Si/n-Si/Ag 구조의 박막 태양전지는 100mW/$cm^2$ 조도 하에서 8.6%의 효율을 나타내었다. ($V_{oc}$=0.85V, $J_{sc}$=16.42mA/$cm^2$, FF=0.615)

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Effects of Neutral Particle Beam on Nano-Crystalline Silicon Thin Film Deposited by Using Neutral Beam Assisted Chemical Vapor Deposition at Room Temperature

  • Lee, Dong-Hyeok;Jang, Jin-Nyoung;So, Hyun-Wook;Yoo, Suk-Jae;Lee, Bon-Ju;Hong, Mun-Pyo
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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    • pp.254-255
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    • 2012
  • Interest in nano-crystalline silicon (nc-Si) thin films has been growing because of their favorable processing conditions for certain electronic devices. In particular, there has been an increase in the use of nc-Si thin films in photovoltaics for large solar cell panels and in thin film transistors for large flat panel displays. One of the most important material properties for these device applications is the macroscopic charge-carrier mobility. Hydrogenated amorphous silicon (a-Si:H) or nc-Si is a basic material in thin film transistors (TFTs). However, a-Si:H based devices have low carrier mobility and bias instability due to their metastable properties. The large number of trap sites and incomplete hydrogen passivation of a-Si:H film produce limited carrier transport. The basic electrical properties, including the carrier mobility and stability, of nc-Si TFTs might be superior to those of a-Si:H thin film. However, typical nc-Si thin films tend to have mobilities similar to a-Si films, although changes in the processing conditions can enhance the mobility. In polycrystalline silicon (poly-Si) thin films, the performance of the devices is strongly influenced by the boundaries between neighboring crystalline grains. These grain boundaries limit the conductance of macroscopic regions comprised of multiple grains. In much of the work on poly-Si thin films, it was shown that the performance of TFTs was largely determined by the number and location of the grain boundaries within the channel. Hence, efforts were made to reduce the total number of grain boundaries by increasing the average grain size. However, even a small number of grain boundaries can significantly reduce the macroscopic charge carrier mobility. The nano-crystalline or polymorphous-Si development for TFT and solar cells have been employed to compensate for disadvantage inherent to a-Si and micro-crystalline silicon (${\mu}$-Si). Recently, a novel process for deposition of nano-crystralline silicon (nc-Si) thin films at room temperature was developed using neutral beam assisted chemical vapor deposition (NBaCVD) with a neutral particle beam (NPB) source, which controls the energy of incident neutral particles in the range of 1~300 eV in order to enhance the atomic activation and crystalline of thin films at room temperature. In previous our experiments, we verified favorable properties of nc-Si thin films for certain electronic devices. During the formation of the nc-Si thin films by the NBaCVD with various process conditions, NPB energy directly controlled by the reflector bias and effectively increased crystal fraction (~80%) by uniformly distributed nc grains with 3~10 nm size. The more resent work on nc-Si thin film transistors (TFT) was done. We identified the performance of nc-Si TFT active channeal layers. The dependence of the performance of nc-Si TFT on the primary process parameters is explored. Raman, FT-IR and transmission electron microscope (TEM) were used to study the microstructures and the crystalline volume fraction of nc-Si films. The electric properties were investigated on Cr/SiO2/nc-Si metal-oxide-semiconductor (MOS) capacitors.

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Solution-Processed Nontoxic and Abundant $Cu_2ZnSnS_4$ for Thin-Film Solar Cells

  • 문주호
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2012년도 춘계학술발표대회
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    • pp.65-65
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    • 2012
  • Copper zinc tin sulfide ($Cu_2ZnSnS_4$, CZTS) is a very promising material as a low cost absorber alternative to other chalcopyrite-type semiconductors based on Ga or In because of the abundant and economical elements. In addition, CZTS has a band-gap energy of 1.4~1.5eV and large absorption coefficient over ${\sim}10^4cm^{-1}$, which is similar to those of $Cu(In,Ga)Se_2$(CIGS) regarded as one of the most successful absorber materials for high efficient solar cell. Most previous works on the fabrication of CZTS thin films were based on the vacuum deposition such as thermal evaporation and RF magnetron sputtering. Although the vacuum deposition has been widely adopted, it is quite expensive and complicated. In this regard, the solution processes such as sol-gel method, nanocrystal dispersion and hybrid slurry method have been developed for easy and cost-effective fabrication of CZTS film. Among these methods, the hybrid slurry method is favorable to make high crystalline and dense absorber layer. However, this method has the demerit using the toxic and explosive hydrazine solvent, which has severe limitation for common use. With these considerations, it is highly desirable to develop a robust, easily scalable and relatively safe solution-based process for the fabrication of a high quality CZTS absorber layer. Here, we demonstrate the fabrication of a high quality CZTS absorber layer with a thickness of 1.5~2.0 ${\mu}m$ and micrometer-scaled grains using two different non-vacuum approaches. The first solution-processing approach includes air-stable non-toxic solvent-based inks in which the commercially available precursor nanoparticles are dispersed in ethanol. Our readily achievable air-stable precursor ink, without the involvement of complex particle synthesis, high toxic solvents, or organic additives, facilitates a convenient method to fabricate a high quality CZTS absorber layer with uniform surface composition and across the film depth when annealed at $530^{\circ}C$. The conversion efficiency and fill factor for the non-toxic ink based solar cells are 5.14% and 52.8%, respectively. The other method is based on the nanocrystal dispersions that are a key ingredient in the deposition of thermally annealed absorber layers. We report a facile synthetic method to produce phase-pure CZTS nanocrystals capped with less toxic and more easily removable ligands. The resulting CZTS nanoparticle dispersion enables us to fabricate uniform, crack-free absorber layer onto Mo-coated soda-lime glass at $500^{\circ}C$, which exhibits a robust and reproducible photovoltaic response. Our simple and less-toxic approach for the fabrication of CZTS layer, reported here, will be the first step in realizing the low-cost solution-processed CZTS solar cell with high efficiency.

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반응성 스퍼트링으로 형성된 ITO의 유전채 소성에 따른 특성변화 (The Property Change of ITO Prepared by Reactive R.F. Sputtering in POP manufacturing Process)

  • 남상옥;지성원;손제봉;허근도;조정수;박정후
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1997년도 하계학술대회 논문집 C
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    • pp.1411-1413
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    • 1997
  • The thin film that is electrically conductive and optically transparent is called conductive transparent thin film. ITO(Indium-Tin Oxide) which is a kind of conductive transparent thin film has been widely used in solar cell, transparent electrical heater, selective optical filter, FDP(Flat Display Panel) such as LCD (Liquid Crystal Display), PDP(Plasma Display Panel) and so on. Especially in PDP, ITO films is used as a transparent electrode in order to maintain discharge and decrease consumption power through the improvement of cell structure. In this study, we prepared ITO by reactive r.f. sputtering with indium-tin(Sn wt 10%) alloy target instead of indium-tin oxide target. The ITO films deposited at low temperature $150^{\circ}C$ and 8% $O_2$ partial pressure showed about $3.6{\Omega}/{\square}$. At the end of firing, the resistance of ITO was decreased, the optical transparence was improved above 90%.

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이중층 몰리브데늄을 후면전극으로 적용한 비진공법 CuInSe2 태양전지의 특성 (Characterization of Non-vacuum CuInSe2 Solar Cells Deposited on Bilayer Molybdenum)

  • 황지섭;윤희선;장윤희;이장미;이도권
    • Current Photovoltaic Research
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    • 제8권2호
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    • pp.45-49
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    • 2020
  • Molybdenum (Mo) thin films are widely used as back contact in copper indium diselenide (CISe) solar cells. However, despite this, there are only few published studies on the properties of Mo and characteristics of CISe solar cells formed on such Mo substrates. In this studies, we investigated the properties of sputter deposited Mo bilayer, and fabricated non-vacuum CISe solar cells using bilayer Mo substrates. The changes in surface morphology and electrical resistivity were traced by varying the gas pressure during deposition of the bottom Mo layer. In porous surface structure, it was confirmed that the electrical resistivity of Mo bilayer was increased as the amount of oxygen bonded to the Mo atoms increased. The resulting solar cell characteristics vary as the bottom Mo layer deposition pressure, and the maximum solar cell efficiency was achieved when the bottom layer was deposited at 7 mTorr with a thickness of 100 nm and the top layer deposited at 3 mTorr with a thickness of 400 nm.