• Title/Summary/Keyword: $CuInS_2$ thin film

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III-V Tandem, CuInGa(S,Se)2, and Cu2ZnSn(S,Se)4 Compound Semiconductor Thin Film Solar Cells (3-5족 적층형과 CuInGa(S,Se)2 및 Cu2ZnSn(S,Se)4 화합물반도체 박막태양전지)

  • Jeong, Yonkil;Park, Dong-Won;Lee, Jae Kwang;Lee, Jaeyoung
    • Applied Chemistry for Engineering
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    • v.26 no.5
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    • pp.526-532
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    • 2015
  • Solar cells with other alternative energies are being importantly recognized related with post-2020 climate change regime formation. In a point of view of materials, solar cells are classified to organic and inorganic solar cells which can provide a plant-scale electricity. In particular, recent studies about compound semiconductor solar cells, such as III-V tandem solar cells, chalcopyrite-series CIGSSe solar cells, and kesterite-series CZTSSe solar cells were rapidly accelerated. In this report, we introduce a research trend and technical issues for the compound semiconductor solar cells.

A Single-Flux-Quantum Shift Register based on High-$T_c$ Superconducting Step-edge Josephson Junctions

  • Sung G.Y.;Choi, C.H.;Suh J.D.;Han, S. K.;Kang, K.Y.;Hwang, J.S.;Yoon, S.G.;Jung, K.R.;Lee, Y.H.;Kang, J.H.;Kim, Y.H.;Hahn, T.S.
    • Progress in Superconductivity
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    • v.1 no.1
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    • pp.31-35
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    • 1999
  • We have fabricated and tested a simple circuit of the rapid single-flux-quantum(RSFQ) four-stage shift register using a single layer high-$T_c$ superconducting (HTS) $YBa_2Cu_3O_{7-x}$ (YBCO) thin film structure with 9 step-edge Josephson junctions. The circuit includes two read superconducting quantum interference devices(SQUID) and four stages. To establish a robust HTS RSFQ device fabrication process, we have focussed on the reproducible process of sharp and straight step-edge formation as well as the ratio of film thickness to step height, t/h. The spread of step-edge junction parameters was measured from each 13 junctions with t/h=1/3, 1/2, and 2/3 at various temperatures. We have demonstrated the simplified operation of the shift register at 65 K.

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Effect of Deposition Rate and Annealing Temperature on Magnetoresistance in Fe$Fe(50{\AA}/[Co(17{\AA})/Cu(24{\AA})]_20$Multilayers (다층박막 $Fe(50{\AA}/[Co(17{\AA})/Cu(24{\AA})]_20$의 증착률 및 열처리가 자기저항에 미치는 효과)

  • 김미양;최수정;최규리;송은영;오미영;이장로;이상석;황도근;박창만
    • Journal of the Korean Magnetics Society
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    • v.8 no.5
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    • pp.282-287
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    • 1998
  • Dependence of magnetoresistance on base pressure and deposition rates of each Fe, Co, Cu layers in the $Fe(50{\AA}/[Co(17{\AA})/Cu(24{\AA})]_20$ multilayer thin films, prepared by dc magnetron sputtering on Corning glass, were investigated. AFM analysis, X-ray diffraction analysis, vibrating sample magnetometer analysis, and magnetoresustance measurement (4-probe method) were performed. The multilayer films deposited under low base pressure increases magnetoresistance ratio by preventing oxidation. Annealing for the samples at a moderate temperature allowed larger textured grain with no loss in the periodicity. Magnetoresistance ratio of the annealed multilayers was increased due to the increase antiferromagnetically coupled fraction of the film after annealing. Optimization of deposition rate was greater than 1 $\AA$/s for Fe, and 2.8 $\AA$/s for Cu. Deposition rate of Co showed a tendency of increasing of magnetoresistance ratio due to the formation of flat magnetic layer in case of high deposition rate of Co.

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Effects of Sodium and Gallium on Characteristics of CIGS Thin Films and CdS/CIGS Solar Cells by Co-evaporation Method (Na확산과 Ga첨가에 따른 동시진공증발법으로 제조된 CIGS 박막과 CdS/CIGS 태양전지의 특성)

  • Kwon, S.H.;Lee, J.C.;Kang, K.H.;Kim, S.K.;Yoon, K.H.;Song, J.S.;Lee, D.Y.;Ahn, B.T.
    • Solar Energy
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    • v.20 no.2
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    • pp.43-54
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    • 2000
  • We prepared and characterized $Cu(In_{1-x}Ga_x)Se_2$(CIGS) films using a elemental co-evaporation method for absorbing layer of high efficiency thin film solar cells. The CIGS films deposited on a soda-lime glass exhibited low resistivity because of higher carrier concentration. Na was accumulated at the CIGS surface and the 0 and Se were also accumulated at the surface, suggesting that oxidation is a driving force of Na accumulation. The structure of CIGS film was modified or a secondary phase was formed in the Cu-poor CIGS bulk films probably due to the incorporation of Na into Cu vacancy sites. As the Ga/(In+Ga) ratio increased, the diffraction peaks of $Cu(In_{1-x}Ga_x)Se_2$ films were shifted to larger angle and splitted, and the grain size of $Cu_{0.91}(In_{1-x}Ga_x)Se_2$ films became smaller. All $Cu_{0.91}(In_{1-x}Ga_x)Se_2$ films showed the p-type conductivity regardless of the Ga/(In+Ga) ratio. Ag/n-ZnO/i-ZnO/CdS/$Cu_{0.91}(In_{0.7}Ga_{0.3})Se_2$/Mo solar cells were fabricated. The currently best efficiency in this study was 14.48% for $0.18cm^2$ area ($V_{oc}=581.5mV,\;J_{sc}=34.88mA$, F.F=0.714).

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Characterization of Cu2ZnSnSe4 Thin Films Selenized with Cu2-xSe/SnSe2/ZnSe and Cu/SnSe2/ZnSe Stacks

  • Munir, Rahim;Jung, Gwang Sun;Ko, Young Min;Ahn, Byung Tae
    • Korean Journal of Materials Research
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    • v.23 no.3
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    • pp.183-189
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    • 2013
  • $Cu_2ZnSn(S,Se)_4$ material is receiving an increased amount of attention for solar cell applications as an absorber layer because it consists of inexpensive and abundant materials (Zn and Sn) instead of the expensive and rare materials (In and Ga) in $Cu(In,Ga)Se_2$ solar cells. We were able to achieve a cell conversion efficiency to 4.7% by the selenization of a stacked metal precursor with the Cu/(Zn + Sn)/Mo/glass structure. However, the selenization of the metal precursor results in large voids at the absorber/Mo interface because metals diffuse out through the top CZTSe layer. To avoid the voids at the absorber/Mo interface, binary selenide compounds of ZnSe and $SnSe_2$ were employed as a precursor instead of Zn and Sn metals. It was found that the precursor with Cu/$SnSe_2$/ZnSe stack provided a uniform film with larger grains compared to that with $Cu_2Se/SnSe_2$/ZnSe stack. Also, voids were not observed at the $Cu_2ZnSnSe_4$/Mo interface. A severe loss of Sn was observed after a high-temperature annealing process, suggesting that selenization in this case should be performed in a closed system with a uniform temperature in a $SnSe_2$ environment. However, in the experiments, Cu top-layer stack had more of an effect on reducing Sn loss compared to $Cu_2Se$ top-layer stack.

Development of High Efficiency CIGS Thin Film Solar Cells (고효율 CIGS 박막 태양전지 개발)

  • Yun, Jae-Ho;Song, Jin-Sub;Kim, Ki-Hwan;Kim, Min-Sik;Ahn, Byung-Tae;Yoon, Kyung-Hoon
    • 한국신재생에너지학회:학술대회논문집
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    • 2006.06a
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    • pp.149-151
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    • 2006
  • Cu계 $I-III-VI_2$화합물은 직접천이형 반도체로 광흡수계수가 매우 높아 박막형 태양전지 제조에 매우 유리하다. 또한 화학적으로 안정하며 Ga, Al 등을 첨가하면 에너지 금지대폭을 조절할 수 있어 Wide Bandgap 태양전지 및 탠덤구조 태양전지를 제조하기에도 용이하다 $CulnSe_2(CIS)$ 물질에서 In을 20-30% 정도 치환한 $Cu(In,Ga)Se_2(CIGS)$ 태양전지의 경우 19.5%의 세계 최고 효율을 보고하고 있으며 이는 다결정 실리콘 태양전지의 효율과 비슷한 수준이다. 본 연구에서는 동시 진공증발법을 이용하여 증착한 CIGS 박막을 이용하여 태양전지를 제조하였다. 공정의 재현성 및 결정립계가 큰 광흡수층 제조를 위하여 실시간 기판온도 모니터링 시스템을 도입하였으며 버퍼충으로는 용액성장한 CdS 박막을 사용하였다. SLG/MO/CIGS(CGS)/CdS/ZnO/Al 구조의 태양전지를 제조하여 면적 $0.5cm^2$에서 각각 17.5%의 효율을 얻었다.

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Characterization of Atomic-Layer Deposited ZnSnO Buffer Layer for 18%- Efficiency Cu(In,Ga)Se2 Solar Cells (18% 효율 Cu(In,Ga)Se2 박막태양전지용 ZnSnO 버퍼층의 원자층 증착법 및 분석)

  • Kim, Sun Cheul;Kim, Seung Tae;Ahn, Byung Tae
    • Current Photovoltaic Research
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    • v.3 no.2
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    • pp.54-60
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    • 2015
  • ZnSnO thin films were deposited by atomic layer deposition (ALD) process using diethyl zinc ($Zn(C_2H_5)_2$) and tetrakis (dimethylamino) tin ($Sn(C_2H_6N)_4$) as metal precursors and water vapor as a reactant. ALD process has several advantages over other deposition methods such as precise thickness control, good conformality, and good uniformity for large area. The composition of ZnSnO thin films was controlled by varying the ratio of ZnO and $SnO_2$ ALD cycles. The ALD ZnSnO film was an amorphous state. The band gap of ZnSnO thin films increased as the Sn content increased. The CIGS solar cell using ZnSnO buffer layer showed about 18% energy conversion efficiency. With such a high efficiency with the ALD ZnSnO buffer and no light soaking effect, AlD ZnSnO buffer mighty be a good candidate to replace Zn(S,O) buffer in CIGSsolar cells.

Characterization of $Cu(In_xGa_{1-x})Se_2$ Solar Cells with Ga Content (Ga 함량에 따른 $Cu(In_xGa_{1-x})Se_2$ 태양전지의 특성분석)

  • Kim, Seok-Ki;Kwon, Se-Han;Lee, Doo-Yeol;Lee, Jeong-Churl;Kang, Ki-Whan;Yoon, Kyung-Hoon;Ahn, Byung-Tae;Song, Jin-Soo
    • Proceedings of the KIEE Conference
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    • 1998.07d
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    • pp.1264-1267
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    • 1998
  • $Cu(In_xGa_{1-x})Se_2$ thin films were prepared and characterized with various Ga contents. As the Ga content increased, the grain size of CIGS film became smaller. The 2 $\theta$ values in XRD patterns were shifted to larger values and the overlapped peaks were splitted. The energy bandgap increased from 1.04 to 1.67 eV and the resistivity decreased. The solar cell fabricated with ZnO/CdS/$Cu(In_{0.7}Ga_{0.3})Se_2/Mo$ structure yielded an efficeincy of 14.48% with an acitive area of 0.18 $cm^2$. The efficiency decreased with further increase of Ga content.

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Photovoltaic Properties of Cu(InGa)$Se_2$ Solar Cells with Sputter Conditions of Mo films (Mo 박막의 성장조건에 따른 Cu(InGa)$Se_2$ 박막 태양전지의 광변환효율)

  • Kim, S.K.;Lee, J.C.;Kang, K.H.;Yoon, K.H.;Park, I.J.;Song, J.;Han, S.O.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.05c
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    • pp.63-66
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    • 2002
  • Bi-layer Mo films were deposited on sodalime glass substrates using DC magnetron sputtering. As the gas pressure and power density, the resistivity varied from $1.5{\times}10^{-5}$ to $4.97{\times}10^{-4}{\Omega}{\cdot}cm$. Furthermore, stress direction yielded compressive-to-tensile transition stress curves. The microstructure of the compressive stress films which had poor adhesion consists of tightly packed columns, but of the tensile-stressed films had less dense structure. Under all gas pressure conditions, Mo films exhibited distinctly increasing optical reflection with decreasing gas pressure. The expansion of (110) peak width with the gas pressure meant the worse crystalline growth. Also, The highest efficiency was 15.2% on 0.2 $cm^2$. The fill factor, open circuit voltage and short circuit current were 63 %, 570 m V and 42.6 $mA/cm^2$ respectively.

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Effects of pH of Reaction Solution on the Structural and Optical Properties of CdS Thin Films for Solar Cell Applications (태양전지용 CdS 박막의 구조적 및 광학적 특성에 미치는 반응용액의 pH 영향)

  • Lee, Jae-Hyeong
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.24 no.8
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    • pp.616-621
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    • 2011
  • In this paper, CdS thin films, which were widely used window layer of the CdTe and the Cu(In,Ga)$Se_2$ thin film solar cell, were grown by chemical bath deposition, and effects of pH of reaction solution on the structural and optical properties were investigated. For pH<10.5, as the pH of reaction solution was higher, the deposition rate of CdS films was increased by improving ion-by-ion reaction in the substrate surface and the crystallinity of the films was improved. However, when the pH was higher than 10.5, the deposition rate was decreased because of smaller $Cd^{2+}$ ion concentration in the reaction solution. Also, the crystallinity of the films were deteriorated. The CdS films deposited at lower pH showed poor optical transmittance due to adsorbed colloidal particles, while the transmittance was improved for higher pH.