• Journal of the Korean Ceramic Society
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• v.45 no.1
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• pp.30-35
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• 2008

In this paper, CdS/Cd(Cu)S thin films and diodes were manufactured via a chemical bath deposition (CBD) process, and the effects of $NH_4Cl$ and TEA(triethylamine) on the properties of the films were examined. The addition of $NH_4Cl$ significantly increased the thickness of the CdS and Cd(Cu)S films, however, the addition of TEA decreased the thickness in both cases slightly. The addition of $NH_4Cl$ along with TEA increased the film thickness more effectively compared to the addition of only $NH_4Cl$. The thickness of the CdS film prepared from an aqueous solution of 0.007 M $CdSO_4$, 1.3 M $NH_4OH$, 0.03 M $SC(NH_2)_2$, 0.0001 M TEA and 0.03 M $NH_4Cl$ was 310 nm. Dark resistivity of the CdS film was $1.2{\times}10^3\;{\Omega}cm$ and the photo resistivity with $500\;W/cm^2$ irradiation of white light was $20{\Omega}cm$. The Cd(Cu)S/CdS thin film diodes prepared by CBD showed good rectifying characteristics.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.08a
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• pp.321.2-321.2
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• 2013

CdS는 2.42 eV의 밴드 갭을 가지는 직접 천이형 반도체로서 CdTe계와 CGIS계 태양전지의 접합 partner로 많이 이용되어 왔다. 태양전지의 광투과층으로 사용되는 CdS 박막의 필요한 물성으로는 높은 광투과도와 얇은 두께이다. 광투과층으로 사용되는 CdS 막의 광투과도가 높아야 많은 양의 빛이 손실 없이 투과하여 광흡수층인 CIGS에 도달할 수 있다. 특히, CdS막의 두께가 얇으면 밴드 갭 이상의 에너지를 가지는 파장의 빛도 투과시킬 수 있어 태양전지의 효율의 증가을 얻을 수가 있다. 그러나 CdS 막의 두께가 얇을 경우, pinhole이 생성되는 등 막의 균질성이 문제가 되기 때문에 얇으면서도 pinhole이 없는 CdS 박막을 만들기 위한 연구가 진행되고 있다. 본 연구에서는 높은 변환 효율을 갖는 CIGS 박막 태양전지 제작에 적합한 chemical bath depostion(츙)법을 이용하여 CdS 박막을 제조하였다. 또한 반응온도, Cd 및 S source 비, 반응용액의 pH와 같은 증착 조건에 따른 박막의 구조적, 광학적 특성을 조사하였다.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.14 no.2
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• pp.104-110
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• 2001

Structural, optical and electrical properties of Cd$_{1-x}$ Zn$_{x}$S films deposited by chemical bath deposition(CBD), which is a very attractive method for low-cost and large-area solar cells, are presented. Especially, in order to control more effectively the zinc component of the films, zinc acetate, which was used as the zinc source, was added in the reaction solution after preheating the reaction solution and the pH of the reaction solution decreased with increasing the concentration of zinc acetate. The films prepared after preheating and pH control had larger zinc component and higher optical band gap. The crystal structures of Cd$_{1-x}$ Zn$_{x}$S films was a wurtzite type with a preferential orientation of the (002) plane and the lattice constants of the films changed from the value for CdS to those for ZnS with increasing the mole ratio of the zinc acetate. The minimum lattice mismatch between Cd$_{1-x}$ Zn$_{x}$S and CdTe were 2.7% at the mole ratio of (ZnAc$_2$)/(CdAc$_2$+ZnAc$_2$)=0.4. As the more zinc substituted for Cd in the films, the optical transmittance improved, while the absorption edge shifted toward a shorterwavelength. the photoconductivity of the films was higher than the dark conductivity, while the ratio of those increased with increasing the mole ratio of zinc acetate. acetate.

• Proceedings of the Korean Vacuum Society Conference
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• 2010.02a
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• pp.294-294
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• 2010

CdS는 $CuInSe_2$계, CdTe계 이종접합 태양전지의 junction partner로 많이 이용되어 왔다. CdS는 전극으로 쓰일 뿐만 아니라 빛을 투과시키는 창문층으로 사용되어 높은 변환 효율을 나타낸다. 이종접합 태양전지에서 창문층은 가시광 영역에서 광투과율이 높고, 전기적으로 비저항이 낮아야 에너지 손실 없이 태양광을 광흡수층까지 투과시킬 수 있다. CdS 박막은 CBD법(solution growth technique), 진공증착법(vacuum evaporation), 스퍼터법(sputtering), 스프레이 열분해법(spray pyrolysis), 전착법(electrodeposition)에 의해 제조되고, 그 중 용액성장법(solution growth technique)이라고도 불리는 CBD법(chemical bath deposition)을 이용하여 CdS 박막을 제조하였다. CBD법은 다른 방법에 비해 제조 과정이 비교적 간단할 뿐만 아니라 제조 단가가 저렴하고, 넓은 면적의 박막 제조가 가능하며 재현성도 우수하다는 장점이 있다. CdS 박막을 제조하기 위한 cadmuim 이온공급원으로는 $CdSO_4$를 사용하였고 sulfur 이온공급원으로는 $SC(NH_2)_2$를 사용하였다. CBD법에서 박막의 물성에 영향을 미칠 수 있는 요인인 sulfur 이온공급원과 cadmium 이온공급원의 비, 용액의 온도, pH를 변화시켜 CdS 박막을 제조하였다. 각각의 조건에 의해 제조된 CdS의 박막의 두께는 Tencor P-1을 이용하여 측정되었고, UV-Visible spectrometer를 이용하여 파장에 따른 광투과율을 측정하였다. CdS 박막의 결정 구조를 조사하기 위해 X선 회절분석(XRD ; X-ray diffraction)을 하였고, AFM(Atomic Force Microscope)으로 표면 특성을 관찰하였다.

• Korean Journal of Materials Research
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• v.22 no.10
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• pp.504-507
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• 2012

Synthesis of RGO (reduced graphene oxide)-CdS composite material was performed through CBD (chemical bath deposition) method in which graphene oxide served as the support and Cadmium Sulfate Hydrate as the starting material. Graphene-based semiconductor photocatalysts have attracted extensive attention due to their usefulness for environmental and energy applications. The band gap (2.4 eV) of CdS corresponds well with the spectrum of sunlight because the crystalline phase, size, morphology, specic surface area and defects, etc., of CdS can affect its photocatalytic activity. The specific surface structure (morphology) of the photocatalyst can be effective for the suppression of recombination between photogenerated electrons and holes. Graphene (GN) has unique properties such as a high value of Young's modulus, large theoretical specific surface area, excellent thermal conductivity, high mobility of charge carriers, and good optical transmittance. These excellent properties make GN an ideal building block in nanocomposites. It can act as an excellent electron-acceptor/transport material. Therefore, the morphology, structural characterization and crystal structure were observed using various analytical tools, such as X-ray diffraction, scanning electron microscopy, transmission electron microscopy, and Raman spectroscopy. From this analysis, it is shown that CdS particles were well dispersed uniformly in the RGO sheet. Furthermore, the photocatalytic property of the resulting RGO-CdS composite is also discussed in relation to environmental applications such as the photocatalytic degradation of pollutants. It was found that the prepared RGO-CdS nanocomposites exhibited enhanced photocatalytic activity as compared with that of CdS nanoparticles. Therefore, better efficiency of photodegradation was found for water purification applications using RGO-CdS composite.

• 한국태양에너지학회:학술대회논문집
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• 2012.03a
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• pp.400-403
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• 2012

$Cu_2ZnSnSe_4$(CZTSe) is emerged as a promising material for thin-film solar cells because of non-toxic, inexpensive and earth abundant more than $Cu(In,Ga)Se_2$ materials. For fabricating compound semiconductor thin-film solar cells, CdS is widely used for a buffer layer which fabricated by a chemical bath deposition method (CBD). Through the experiment, we controlled deposition temperature and mol ratio of solution conditions to find the proper grain 크기 and exact composition. The optimum CdS layers were characterized in terms of surface morphology by using a scanning electron microscope (SEM) and atomic force microscope (AFM). The optimized CdS layer process was applied on CZTSe thin-films. The thickness of buffer layer related with device performance of solar cells which controlled by deposition time. Local surface potential of CdS/CZTSe thin-films was investigated by Kelvin probe force microscopy (KPFM). From these results, we can deduce local electric properties with different thickness of buffer layer on CZTSe thin-films. Therefore, we investigated the effect of CdS buffer layer thickness on the CZTSe thin-films for decreasing device losses. From this study, we can suggest buffer layer thickness which contributes to efficiencies and device performance of CZTSe thin-film solar cells.

• JSTS:Journal of Semiconductor Technology and Science
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• v.15 no.2
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• pp.267-275
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• 2015

In this paper, ZnO films were prepared by atomic layer deposition (ALD) and CdS films were deposited using chemical bath deposition (CBD) to form ZnO/CdS heterojunction. More accurate mapping of band arrangement of the ZnO/CdS heterojunction has been performed by analyzing its electrical and optical characteristics in depth by various methods including transmittance, x-ray photoemission spectroscopy (XPS), and ultraviolet photoemission spectroscopy (UPS). The optical bandgap energies ($E_g$) of ZnO and CdS were 3.27 eV and 2.34 eV, respectively. UPS was capable of extracting the ionization potential energies (IPEs) of the materials, which turned out to be 8.69 eV and 7.30 eV, respectively. The electron affinity (EA) values of ZnO and CdS calculated from IPE and $E_g$ were 5.42 eV and 4.96 eV, respectively. Energy-band structures of the heterojunction could be accurately drawn from these parameters taking the conduction band offset (CBO) into account, which will substantially help acquisition of the full band structures of the thin films in the CIGS solar-cell device and contribute to the optimal device designs.

• Journal of the Korean institute of surface engineering
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• v.29 no.6
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• pp.862-868
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• 1996

Cadmium sulfide is commonly used as the window material for thin film solar cells, and can be prepared by several techniques such as sputtering, spray pyrolysis, close spaced sublimation (CSS), thermal evaporation, solution growth methods, etc. In this study, CdS films were deposited by thermal evaporation, close spaced sublimation, and solution growth methods, respectively, and the effects of the methods on physical properties of polycrystalline CdS deposited on ITO/glass were investigated. Also, the effects of variously prepared CdS thin films on the physical properties of CdTe deposited on the CdS were investigated. The thickness of polycrystalline CdS films was maintained at $0.3\mu\textrm{m}$ except for the solution grown CdS when $0.2\mu\textrm{m}$ thick CdS was deposited. After the deposition, all the samples were annealed at $400^{\circ}C$ or $500^{\circ}C$ in H2 atmosphere. To investigate physical properties of the deposited and annealed CdS thin films, UV-VIS spectro-photometry, X-ray diffractometry (XRD), and Auger electron spectroscopy (AES), and cross sectional transmission electron microscopy(XTEM) were used to analyze grain size, crystal structure, preferred orientation, optical properties, etc. The annealed CdS showed the bandedge transition at 510nm and the optical transmittance high than 80% for all of the variously deposited films. XRD results showed that CdS thin films variously deposited and annealed had the same hexagonal structures, however, showed different preferred orientations. CSS grown CdS had [103] preferred orientation, thermally evaporated CdS had [002], and CdS grown by the solution growth had no preferred orientation. The largest grain size was obtained for the CSS grown CdS while the least grain size was obtained for the solution grown CdS. Some of the physical properties of CdTe deposited on the CdS thin film such as grain size at the junction and grain orientation were affected by the physical properties of CdS thin films.

• Proceedings of the Materials Research Society of Korea Conference
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• 1998.05a
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• pp.99-99
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• 1998

• Proceedings of the Materials Research Society of Korea Conference
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• 2010.05a
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• pp.35.2-35.2
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• 2010

최근 $Cu(In,Ga)Se_2$(CIGS)와 같은 박막 태양전지에 대한 연구가 많은 관심을 끌고 있다. CIGS 태양전지의 광투과층으로 사용되고 있는 II-VI족 화합물 반도체인 CdS는 상온에서의 에너지 밴드 갭(band gap)이 2.42eV 정도로서, 가시광영역의 많은 빛을 투과시키고, 적절한 제작 조건하에서 비교적 낮은 비저항을 나타내기 때문에 널리 사용되고 있다. 하지만 CIGS 태양전지 연구는 주로 CIGS 흡수층 제조공정에 편중되어 있으며, CdS 버퍼층 공정조건에 대한 체계적인 연구가 부족하다고 판단된다. 습식공정인 Chemical Bath Deposition (CBD)에 의해 주로 제조되는 CdS는 단순한 제조공정에도 불구하고 CIGS 태양전지의 성능에 지대한 영향을 미치는 것으로 알려져 있다. 특히, CdS합성반응이 개시되기 전까지의 용액잔류시간 (dip time)은 CIGS내로의 Cd이온 농도를 결정하는 중요한 공정변수로 판단된다. CIGS 표면에 Cd이 도핑될 경우, CIGS는 n형 전도성을 갖는 얇은 층을 갖게 되어 전체적으로 n-CIGS/p-CIGS의 동종 접합을 형성하는 장점을 부여할 것으로 기대된다. 따라서 본 논문에서는 dip time을 주요변수로 하여 CIGS 태양전지의 성능에 미치는 영향을 주로 고찰하였다. Cd의 확산 정도는 secondary ion mass spectroscopy (SIMS)를 이용하여 정량화하였으며, 제조된 CIGS 태양전지의 전류-전압 특성과 상관성을 제시하고자 한다.