• 제목/요약/키워드: $CU(InGa)Se_2$film

검색결과 152건 처리시간 0.034초

Characterization of an In2Se3 Passivation Layer for CIGS Solar Cells with Cd-free Zn-containing Atomic-layer-deposited Buffers

  • Kim, Suncheul;Lee, Ho Jin;Ahn, Byung Tae;Shin, Dong Hyeop;Kim, Kihwan;Yun, Jae Ho
    • Current Photovoltaic Research
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    • 제9권3호
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    • pp.96-105
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    • 2021
  • Even though above 22% efficiencies have been reported in Cd-free Cu(In,Ga)Se2 (CIGS) solar cell with Zn-containing buffers, the efficiencies with Zn-containing buffers, in general, are well below 20%. One of the reasons is Zn diffusion from the Zn-containing buffer layer to CIGS film during buffer growth. To avoid the degradation, it is necessary to prevent the diffusion of Zn atoms from Zn-containing buffer to CIGS film. For the purpose, we characterized an In2Se3 film as a possible diffusion barrier layer because In2Se3 has no Zn component. It was found that an In2Se3 layer grown at 300℃ was very effective in preventing Zn diffusion from a Zn-containing buffer. Also, the In2Se3 had a large potential barrier in the valence band at the In2Se3/CIGS interface. Therefore, In2Se3 passivation has the potential to achieve a super-high efficiency in CIGS solar cells that employ Cd-free ALD processed buffers containing Zn.

Hot Walll Epitaxy (HWE)법에 의한 $CuInSe_2$ 단결정 박막 성장과 가전자대 갈라짐에 대한 광전류 연구 (Growth and Photocurrent Study on the Splitting of the Valence Band for $CuInSe_2$ Single Crystal Thin Film by Hot Wall Epitaxy)

  • 윤석진;홍광준
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2004년도 추계학술대회 논문집 Vol.17
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    • pp.234-238
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    • 2004
  • A stoichiometric mixture of evaporating materials for $CuInSe_2$ single crystal thin films was prepared from horizontal electric furnace. To obtain the single crystal thin films, $CuInSe_2$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the hot wall epitaxy (HWE) system. The source and substrate temperatures were $620^{\circ}C$ and $410^{\circ}C$, respectively. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $CuInSe_2$ single crystal thin films measured with Hall effect by van der Pauw method are $9.62{\times}10^{l6}\;cm^{-3}$ and $296\;cm^2/V{\cdot}s$ at 293 K, respectively. The temperature dependence of the energy band gap of the $CuInSe_2$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)\;=\;1.1851\;eV\;-\;(8.99{\times}10^{-4}\;eV/K)T^2/(T+153K)$. The crystal field and the spin-orbit splitting energies for the valence band of the $CuInSe_2$ have been estimated to be 0.0087 eV and 0.2329 eV at 10K, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the ${\Delta}_{so}$ definitely exists in the $\Gamma_6$ states of the valence band of the $CuInSe_2$. The three photocurrent peaks observed at 10K are ascribed to the $A_1-$, $B_1-$, and $C_1$-exciton peaks for n = 1.

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Al 그리드와 ZnO 투명전도막 의 공정변화에 따른 Cu(In,Ga)Se2 박막태양전지의 특성 연구 (Effect of Process Variation of Al Grid and ZnO Transparent Electrode on the Performance of Cu(In,Ga)Se2 Solar Cells)

  • 조보환;김선철;문선홍;김승태;안병태
    • Current Photovoltaic Research
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    • 제3권1호
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    • pp.32-38
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    • 2015
  • CIGS solar cell consisted of various films. In this research, we investigated electrode materials in $Cu(In,Ga)Se_2$ (CIGS) cells, including Al-doped ZnO (ZnO:Al), intrinsic ZnO (i-ZnO), and Al films. The sputtered ZnO:Al film with a sputtering power at 200W showed the lowest series resistance and highest cell efficiency. The electrical resistivity of the 200-W sputtered ZnO:Al film was $5.2{\times}10^{-4}{\Omega}{\cdot}cm$ by the rapid thermal annealing at $200^{\circ}C$ for 1 min. The electrical resistivity of i-ZnO was not measurable due to its high resistance. But the optical transmittance was highest with less oxygen supply and high efficiency cell was achieved with $O_2/(Ar+O_2)$ ratio was 1% due to the increase of short-circuit current. No significant change in the cell performance by inserting a Ni layer between Al and ZnO:Al films was observed.

CuInGaSe2 단일 타겟을 이용한 대면적 CIGS 스퍼터링 박막의 특성 (Characteristics of large-area CIGS thin films fabricated by sputtering CuInGaSe2 single target)

  • 김태원;김영백;송상인;박재철
    • 한국신재생에너지학회:학술대회논문집
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    • 한국신재생에너지학회 2011년도 춘계학술대회 초록집
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    • pp.125.2-125.2
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    • 2011
  • CuInGaSe2 (CIGS)을 포함한 Chalcopyrite계 물질은 직접천이형 반도체이면서, ${\sim}1{\times}10^5cm^{-1}$ 이상의 광흡수계수를 보이며, 조성제어를 통한 밴드갭 조절이 가능해 차세대 고효율 박막태양전지재료로 매우 주목받고 있다. 최근, CIGS 박막태양전지 제조를 위해 CIGS 흡수층의 여러 가지 박막제조 공정들이 개발되고 있으나, 동시증착법과 소위 2단계법이라 일컬어지는 금속 전구체 스퍼터링 증착 후 셀렌화 공정을 가장 대표적인 공정이라 말 할 수 있다. 동시증착법은 실험실 수준의 소면적 셀에서 20%에 가까운 높은 효율의 CIGS 박막태양전지 제조에 성공하였음에도 불구하고, 상용화를 위한 대면적 셀 제조를 위해 해결해야 할 문제들이 아직 남아있다. 또한, 2단계법의 경우는 스퍼터링 공정을 기반으로 대면적 셀 제조에는 용이하나, CIGS/Mo 계면에서의 Ga 응집현상의 발생 및 셀렌화 공정에 사용되는 독성가스($H_2Se$)의 문제 등이 남아 있어 새로운 시각에서의 접근 방법이 요구되고 있다. 본 연구에서는 CIGS 4성분계 단일 타겟을 사용, RF 스퍼터링 공정을 통해 $200{\times}200mm^2$ 기판 위에 CIGS 박막을 제조하여 그 특성을 분석하였다. XRD 분석결과, 동시증착법에서 일반적으로 관찰되는 CIGS/Mo 계면에서의 $MoSe_2$ 상의 존재는 관찰되지 않았으며, CIGS 단일상의 다결정 박막이 제조되었음을 알 수 있었다. 또한, CIGS 박막제조 후, RTA 공정을 통해 CIGS 박막의 결정성이 향상됨을 관찰 할 수 있었으며, SIMS 분석결과, Mo층의 공정 조건에 따라 CIGS/Mo 계면에서의 금속원소 (In, Ga, Mo)의 상호확산이 크게 억제됨을 알 수 있었다. 그 외의 특성평가 결과들을 통하여 CIGS 4성분계 단일 타겟을 사용한 CIGS 박막태양전지 제조의 유용성에 대해 논의하고자 한다.

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

  • 김석기;이정철;강기환;윤경훈;박이준;송진수;한상옥
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2002년도 춘계학술대회 논문집 유기절연재료 전자세라믹 방전플라즈마 일렉트렛트 및 응용기술
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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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Electrical Characterization of Cu(InxGa1-x)(SySe2-y) Thin Film Solar Cells

  • Kim, Dahye;Kim, Ji Eun;Cho, Yunae;Kim, Dong-Wook
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.464.1-464.1
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    • 2014
  • Among numerous material candidates, Cu(InxGa1-x)(SySe2-y) (CIGS) thin films have emerged as promising material candidates for thin film solar cell applications due to the high energy conversion efficiency and relatively low fabrication cost. The CIGS thin film solar cells consist of several materials, including Mo back contacts, ZnO-based window layers, and CdS buffer layers. All these materials have different crystal structures and contain quite distinct chemical elements, and hence the device characterization requires careful analyses. Most of all, identification of the major trap states resulting in the carrier recombination processes is a key step toward realization of high efficiency CIGS solar cells. We have carried out electrical investigations of CIGS thin film solar cells to specify the major trap states and their roles in photovoltaic performance. In particular, we have used the temperature-dependent transport characterizations and admittance spectroscopy. In this presentation, we will introduce some exemplary studies of DC and AC electrical characteristics of the CIGS solar cells.

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투명 전도막 개선을 통한 Cu(Inx,Ga1-x)Se2 박막태양전지 효율 향상에 관한 연구 (Improvement of Efficiency of Cu(Inx,Ga1-x)Se2 Thin Film Solar Cell by Enhanced Transparent Conductive Oxide Films)

  • 김기림;손경태;김민영;조성희;신준철;임동건
    • 한국전기전자재료학회논문지
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    • 제27권4호
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    • pp.203-208
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    • 2014
  • In this study, Sputtering method was used to grow Al-dopes ZnO films on a CIGS absorber layer, in order to examine the effect of TCO on properties of CIGS solar cell devices. Structural, electrical and optical properties were investigated by varied thickness of Al-dopes ZnO films. Also, relation to the application as a window layer in CIGS thin film solar cell were studied. It was found that the electrical and structural properties of ZnO:Al film improved with increasing its thickness. However, the optical properties degraded. Jsc of the fabricated CIGS based solar cells was significantly influenced by the variation of the ZnO:Al window layer thickness. Because ZnO:Al window layer is one of the Rs factors in CIGS solar cell. Rs has the biggest influence on efficiency characteristic. In order to obtain high efficiency of CIGS solar cell, ZnO:Al window layer should be fabricated with electrically and optically optimized.

Cu(InGa)Se$_2$ 박막의 성장온도에 따른 태양전지의 광전특성 분석 (Photovoltaic Properties of Solar Cells with Deposition Temperature of Cu(InGa)Se$_2$ Films)

  • 김석기;이정철;강기환;윤경훈;박이준;송진수;한상옥
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2002년도 하계학술대회 논문집
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    • pp.330-333
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    • 2002
  • The substrate temperature is an important parameter in thin film deposition process. In this paper the effects of the substrate temperature on the properties of CuIn0.75Ga0.25Se2(CIGS) thin films are reported. Structure, surface morphology and optical properties of CIGS thin films deposited at various substrate temperatures have been investigated using a number of analysis techniques. X-ray diffraction (XRD) analysis shows that CIGS films exhibit a strong <112> preferred orientation. As expected, at higher substrate temperatures the films displayed a higher degree of crystallinity. The <112> peak was also enhanced and other CIGS peaks appeared simultaneously These results were supported by experimental work using Raman spectroscopy. The Raman spectra of the as-grown CIGS thin films show only the Al mode peak. The intensity of this peak was enhanced at higher deposition temperatures. Scanning electron microscopy (SEM) results revealed very small grains in films fabricated at 48$0^{\circ}C$ substrate temperature. When the substrate temperature was increased the average grain size also increased together with a reduction in the number and size of the voids. The deposition temperature also had a significant influence on the transmission spectra.

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$CuAlSe_2$ 단결정 박막의 성장과 광전류 특성 (Growth and Photocurrent Properties for $CuAlSe_2$ Single Crystal Thin film)

  • 홍광준;백승남
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2004년도 추계학술대회 논문집 Vol.17
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    • pp.226-229
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    • 2004
  • A stoichiometric mixture of evaporating materials for $CuAlSe_2$ single crystal thin films was prepared from horizontal electric furnace. To obtain the single crystal thin films, $CuAlSe_2$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the hot wall epitaxy (HWE) system. The source and substrate temperatures were $680^{\circ}C$ and $410^{\circ}C$, respectively. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $CuAlSe_2$ single crystal thin films measured with Hall effect by van der Pauw method are $9.24{\times}10^{16}\;cm^{-3}$ and $295\;cm^2/V{\cdot}s$ at 293 K, respectively. The temperature dependence of the energy band gap of the $CuAlSe_2$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)\;=\;2.8382\;eV\;-\;(8.68{\times}10^{-4}\;eV/K)T^2/(T+155K)$. The crystal field and the spin-orbit splitting energies for the valence band of the $CuAlSe_2$ have been estimated to be 0.2026 eV and 0.2165 eV at 10K, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the ${\Delta}so$ definitely exists in the ${\Gamma}_5$ states of the valence band of the $CuAlSe_2$. The three photocurrent peaks observed at 10K are ascribed to the $A_1-$, $B_1-$, and $C_1$-exciton peaks for n = 1.

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