• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.295-295
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• 2011

CIGS박막을 동시 증발법(co-evaporation)으로 몰리브덴이 증착된 소다라임 유리 위에 성장시켰다. CdS 박막은 화학적 용액 성장법 (chemical bath deposition: CBD)을 이용하여 약 60 nm를 증착하였다. 열처리는 가열판 (hot-plate)을 사용하여 공기중에서 하였다. 열처리 온도는 0~350$^{\circ}C$까지 변화하였으며, 열처리 시간은 각각 5분이었다. 시료의 표면 및 계면의 변화를 SEM측정을 통하여 관측하였다. CdS/CIGS 박막의 열처리 온도 변화에 따른 photoluminescence 특성을 조사하였다. 여기 레이저는 488 nm ($Ar^+$ laser)와 632.8 nm (He-Ne laser)를 사용하여 결함의 근원을 조사하였다. 온도 의존성 실험을 통하여 CIGS 박막의 띠 간격 에너지를 확인할 수 있었으며, 결함 준위의 활성화 에너지 및 특성을 알 수 있었다. $Ar^+$ laser에서만 관측되는 신호의 근원은 CdS에 기인한 것이었다.

• Journal of the Microelectronics and Packaging Society
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• v.26 no.4
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• pp.107-111
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• 2019

We report the fabrication of a CdS/CuInGaSe (CdS/CIGS) structure with carbon nanotubes and its application as a photocathode for photoelectrochemical water splitting. CIGS thin films were fabricated using co-evaporation by RF magnetron sputtering, while CdS was fabricated by chemical bath deposition. Spray coated multi-wall carbon nanotube (CNT) film on CdS/CIGS thin film was investigated as a photocathode. The CNT-coated CdS/CIGS showed superior photocurrent density and exhibited improved photostability.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2004.07a
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• pp.276-279
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• 2004

CdS thin films on polymer substrates such as polycarbonate(PC) and polyethylene terephthalat(PET) have many merits such as light weight, small volume and can make the obtained devices folded, easily carried. In present work, CdS thin films on glass, PC, and PET substrates have been prepared by chemical bath deposition. The structural and optical propertied of the films depending on substrate types have been investigated.

• Progress in Superconductivity and Cryogenics
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• v.8 no.4
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• pp.19-21
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• 2006

Biaxially textured Ni was fabricated by electrodeposition process and delaminated from the biaxially textured cathode surface for further buffer layer deposition process. Those electrode posited Ni substrates showed well-developed biaxial texture and smooth surface. In order to improve the thermal stability of Ni substrates, Mn was alloyed by adding Mn precursor into the electrodeposition bath. Subsequently, $CeO_2$ buffer layers are deposited by MOD process to prevent interfacial reaction between superconductor and substrates. In particular, Bismuth oxide was added to $CeO_2$ to realize lower temperature processing of buffer layers. The microstructure and texture development of each layers have been investigated. Preliminary results shows that all electro/chemical process can be a candidate for cost effective route to YBCO coated conductor.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2008.06a
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• pp.228-228
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• 2008

CdS is II-VI semiconductor with a wide band gap of approximately 2.42 eV. CdS is the most popularly employed heterojunction partner to p-CdTe due to its similar chemical properties. In this work, to improvement of the surface properties of the CdS films, PET substrate is treated by high density $O_2$ plasma. CdS films are prepared by chemical bath deposition(CBD) method. In case of the PET substrate with plasma treatment for 2min, the crystalline orientation of CdS films exhibits a strong hexagonal(002). Grain size was increased from 300nm without $O_2$ plasma treatment to 380nm with an $O_2$ plasma treatment.

• Journal of Sensor Science and Technology
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• v.10 no.1
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• pp.62-70
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• 2001

The ZnSe sample grown by chemical bath deposition (CBD) method were annealed in Ar gas at $45^{\circ}C$. Using extrapolation method of X-ray diffraction pattern, it was found to have zinc blend structure whose lattice parameter $a_o$ was $5.6687\;{\AA}$. From Hall effect, the mobility was likely to be decreased by impurity scattering at temperature range from 10 K to 150 K and by lattice scattering at temperature range from 150 K to 293 K. The band gap given by the transmission edge changed from $2.700{\underline{5}}\;eV$ at 293 K to $2.873{\underline{9}}\;eV$ at 10 K. Comparing photocurrent peak position with transmission edge, we could find that photocurrent peaks due to excition electrons from valence band, ${\Gamma}_8$ and ${\Gamma}_7$ and to conduction band ${\Gamma}_6$ were observed at photocurrent spectrum. From the photocurrent spectra by illumination of polarized light on the ZnSe thin film, we have found that values of spin orbit coupling splitting ${\Delta}so$ is $0.098{\underline{1}}\;eV$. From the PL spectra at 10K, the peaks corresponding to free bound excitons and D-A pair and a broad emission band due to SA is identified. The binding energy of the free excitons are determined to be $0.061{\underline{2}}\;eV$ and the dissipation energy of the donor -bound exciton and acceptor-bound exciton to be $0.017{\underline{2}}\;eV$, $0.031{\underline{0}}\;eV$, respectively.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.684-685
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• 2013

p-형 반도체인 Cu(In,Ga)$Se_2$ (CIGS) 광 흡수 층은 이보다 에너지 밴드 간격이 큰 n-형 반도체와 이종 접합을 형성한다. 흡수층과 윈도우층 사이의 결정구조 차이와 밴드갭 에너지 차이를 완화시키기 위해 버퍼층이 필요하다. 버퍼층을 형성하는 물질로 화학적 용액 성장법(Chemical Bath deposition)을 사용한 CdS가 많이 적용되어 왔으나 Cd의 유해성 및 습식 공정으로 인한 연속공정에 대한 어려움이 있다. 따라서 버퍼층을 Cd을 포함하지 않는 ZnS, $In_2S_3$, (Zn, Mg)O 등과 같은 물질로 대체하여 원자층 증착법(Atomic Layer Deposition), 펄스레이져증착법(Pulsed Laser Deposition), 스퍼터링(sputtering) 등과 같은 건식으로 성장시키는 연구가 활발히 진행되고 있다. 본 연구에서는 $ZnO_{1-x}S_x$ ($0.2{\leq}x{\leq}0.4$)를 반응성 스퍼터링으로 증착하여 큰 밴드갭 에너지와 높은 광투과율를 갖는 버퍼층을 제작하였다. CIGS 박막의 손상을 줄여주기 위하여 RF 파워는 240, 200, 150, 100 W로 변화시켰다. CIGS 태양전지의 I-V 측정 결과, RF 파워가 150 W일 때 10.7%의 가장 높은 변환 효율을 보였고, 150 W 이상에서는 파워가 증가할 때 단락전류는 감소하였으며 개방전압은 다소 증가하였다. 반면 100 W에서 단락전류는 다소 증가하는 것에 반해 개방 전압이 급격히 낮아졌다. 이것은 파워에 따라 결합되는 산소의 양이 다르기 때문으로 생각된다.

• Journal of the Korean institute of surface engineering
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• v.37 no.2
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• pp.80-85
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• 2004

Chromium-carbon (Cr-C) and chromium-carbon-phosphorus (Cr-C-P) alloy deposits using trivalent chromium sulfate baths containing potassium formate were prepared to study their current efficiency, hardness change and phase transformations behavior with heat treatment, respectively. The current efficiencies of Cr-C and Cr-C-P alloy deposits increase with increasing current density in the range of 15-35 A/dm$^2$. Carbon content of Cr-C and phosphorous of Cr-C-P layers decreases with increasing current density, whereas, the carbon content of Cr-C-P layer is almost constant with the current density. Cr-C deposit shows crystallization at $400^{\circ}C$ and has (Cr+Cr$_{ 23}$$C_{6}$) phases at $800^{\circ}C$. Cr-C-P deposit shows crystallization at $600^{\circ}C$ and has (Cr+Cr$_{23}$ $C_{6}$$+Cr_3$P) phases at $800^{\circ}C$. The hardness of Cr-C and Cr-C-P deposits after heating treatment for one hour increase up to Hv 1640 and Hv 1540 and decrease about Hv 820 and Hv 1270 with increasing annealing temperature in the range of $400～^{\circ}C$, respectively. The hardness change with annealing is due to the order of occurring of chromium crystallization, precipitation hardening effect, softening and grain growth with temperature. Less decrease of hardness of Cr-C-P deposit after annealing above $700^{\circ}C$ is related to continuous precipitation of $Cr_{23}$ $C_{6}$ and $Cr_3$P phases which retard grain growth at the temperature.

• Proceedings of the Korean Vacuum Society Conference
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• 2012.08a
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• pp.171-171
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• 2012

We have studied the effects of plasma treatments on CdS buffer layers in CIGS thin film solar cells. The CdS layers were deposited on CIGS films by chemical bath deposition (CBD) method. The RF plasma treatments of the CdS thin films were performed with Ar, $O_2 and $N_2 gases, respectively. After plasma treatments, the solar cells with Al:ZnO/i-ZnO/CdS/CIGS structures were fabricated. The surface properties of the CdS/CIGS thin films after plasma treatments were investigated with SEM, EDX and AFM measurements. The electrical properties of manufactured solar cell were discussed with the results of current-voltage measurements. The plasma treatments have a strong influence on the open circuit voltage (VOC) and the fill factor of the solar cells. Finally, a correlation between the surface properties of CdS layer and the efficiencies of the CIGS thin film solar cells is discussed.

• 한국신재생에너지학회:학술대회논문집
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• 2011.05a
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• pp.106.2-106.2
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• 2011

다층 박막 구조로 이루어진 CdS/CdTe 태양전지의 경우, 각각의 박막이 다양한 제조 공정을 거치면서 물성특성의 변화를 겪게 된다. 각각의 박막이 고온의 열처리 공정과, $CdCl_2$ 용액 처리 및 후면 산화막 제거 공정 등을 거치게 되면서 겪게 되는 물성 변화 분석을 살펴보고자 한다. 각각의 박막 제조 방식은 일반적으로 사용되는 방식으로, CdS의 경우는 용액성장법(Chemical Bath Deposition, CBD), CdTe의 경우는 근접승화법(Closed Space Sublimaition, CSS)을 사용했으며, X-Ray Diffractometer (XRD), Raman spectroscopy, Field Emission Scanning Electron Microscope (FE-SEM), Energy Dispersive Spectroscopy (EDS), X-ray Photoelectron Spectroscopy (XPS) 등을 이용하여 분석하였다. 각각의 셀 제조 공정을 거치면서 CdS, CdTe 박막들은 결정, 광 특성, 성분 변화를 보였다.