• 센서학회지
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• 제2권1호
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• pp.81-86
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• 1993

Chemical bath deposition 방법으로 다결정 CdSe 박막을 세라믹 기판 위에 성장시킨 다음 온도를 변화시켜 열처리하고 X-선 회절무늬를 측정하여 결정구조를 밝혔다. $450^{\circ}C$로 열처리한 시료가 X-선 회절무늬로 부터 외삽법에 의해 $a_{o}$와 $c_{o}$는 각각 $4.302{\AA}$과 $7.014{\AA}$인 육방정계임을 알았다. 이 때 낱알크기는 약 $0.3{\mu}m$이었다. Van der Pauw 방법으로 Hall 효과를 측정하여 운반자 농도와 이동도의 온도의존성을 연구하였다. 이동도는 33 K에서 200 K까지는 압전산란에 의하여, 200K에서 293 K까지는 극성광학산란에 의하여 감소하는 경향을 나타냈다. 광전도 셀의 특성으로 스텍트럼 응답, 감도(${\gamma}$), 최대허용소비전력 및 응답 시간을 측정하였다.

• 한국태양에너지학회:학술대회논문집
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• 한국태양에너지학회 2012년도 춘계학술발표대회 논문집
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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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• 제15권2호
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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.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2008년도 하계학술대회 논문집 Vol.9
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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.

• KEPCO Journal on Electric Power and Energy
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• 제1권1호
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• pp.175-180
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• 2015

본 연구에서는 간단한 화학적 합성 방법을 통하여 스테인레스 기판 위에 nano-bud 형태의 수산화 구리 박막을 형성하였다. 그리고 또 다른 합성 방법인 chemical bath deposition을 이용하여 수산화 구리 나노 구조를 간단하고 친환경적으로 형성하였다. 수산화 구리 박막의 구조적 연구는 X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), field emission scanning electron microscopy (FESEM) 방법을 통하여 이루어졌으며 다결정의 nano-bud 형상을 확인할 수 있었다. 또한 나노 구조로 합성된 수산화구리 전극의 전기화학적 측정은 1M KOH의 전해질 조건에서 cyclic voltammetry (CV) and galvanostatic charge-discharge (GCD)에서 측정되었으며 $340Fg^{-1}$의 높은 비 용량을 보였다. 또한 $1mA\;cm^{-2}$ 의 전력 밀도에서 ${\sim}83Wh\;kg^{-1}$의 높은 에너지 밀도와 ${\sim}3.1kW\;kg^{-1}$의 높은 출력 밀도를 가지며 향상된 전극의 성능을 보였다. 이러한 뛰어난 의사 캐패시터의 성능은 수산화 구리의 nano-bud 형상에 의한 효과로 확인할 수 있었다. 본 연구를 통하여 화학적 합성 방법의 확장을 통하여 수산화 구리 전극의 에너지 저장 장치로써의 성능을 확인할 수 있었다.

• 태양에너지
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• 제17권2호
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• pp.55-66
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• 1997

CdTe/CdS 태양전지 제작에 필요한 다결정 CdS 박막을 ITO 전도 유리기판위에 SSD법, SPD법 및 CBD법 으로 제작하고 열처리 한 후 그 결정구조와 광학적 특성을 조사하였다. 박막은 모두 Wurtzite 구조를 보였고 SSD법과 CBD법의 박막은 $0.5{\mu}m$ 크기의 CdS 입자가 불규칙적으로 형성되어 증착되어 있음을 보였고, $400^{\circ}C$로 진공중에서 열처리 할 때 입자의 크기가 약간 증가하였다. SPD법의 박막은 (002)방향으로 결정이 성장되고 입자의 크기가 $0.1-0.3{\mu}m$ 이었다. 에너지 밴드갭 및 결함 상태를 광학적 흡수, 광 루미니센스, 라만 및 광 열 편기 스펙트럼(PDS) 측정을 통해 조사하였다.

• 한국전기전자재료학회논문지
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• 제14권5호
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• pp.423-429
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• 2001

PbS, CuS and (Pb,Cu)S thin films were chemically deposited on glass from alkaline baths containing lead acetate, copper chloride, thiourea and triethanolamine. The deposition, optical, resistivity and thermal electric properties of these films were studied. PbS thin films showed a hexagonal structure and CuS thin films showed amorphous. The crystalline of (Pb,Cu)S thin films was obtained by heat treatment at 200$\^{C}$ and the deposition ratio of Pb to Cu showed 7:3. The energy gap of PbS, CuS and (Pb,Cu)S thin films were 1.7, 2.1 and 2.4 eV, respectively. Sheet resistance of PbS thin films was less affected on thermal annealing, but hose of (Pb,Cu)S and CuS thin films were more reduced about 3 orders of magnitude. All of those thin films indicated p type semiconductor in temperature ranging 30$\^{C}$ to 150$\^{C}$.

• 한국신재생에너지학회:학술대회논문집
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• 한국신재생에너지학회 2011년도 춘계학술대회 초록집
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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.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.533-538
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• 2001

The ZnSe sample grown by chemical bath deposition (CBD) method were annealed in Ar gas at 450$^{\circ}C$ 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 29 3K. The band gap given by the transmission edge changed from 2.7005 eV at 293 K to 2.8739 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/ 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 Δso is 0.0981 eV. From the PL spectra at 10 K, 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 0.0612 eV and the dissipation energy of the donor -bound exciton and acceptor-bound exciton to be 0.0172 eV, 0.0310 eV, respectively.

• Advances in materials Research
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• 제12권3호
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• pp.179-192
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• 2023

We have studied the structural and optical properties of the non-doped and Co 0.08 at.%, Co 0.02 at.%, and Co 0.11 at.% doped ZnO nanorods (NRs) synthesized using the simple low-temperature chemical bath deposition (CBD) method at 95℃ for 2 hours. The scanning electron microscope (SEM) images confirmed the morphology of the ZnO NRs are affected by Co incorporation. As observed, the Co 0.08 at.% doped ZnO NRs have a larger dimension with an average diameter of 153.4 nm. According to the International Centre for Diffraction Data (ICDD) number #00-036-1451, the x-ray diffraction (XRD) pattern of non-doped and Co-doped ZnO NRs with the preferred orientation of ZnO NRs in the (002) plane possess polycrystalline hexagonal wurtzite structure with the space group P63mc. Optical absorbance indicates the Co 0.08 at.% doped ZnO NRs have stronger and blueshift bandgap energy (3.104 ev). The room temperature photoluminescence (PL) spectra of ZnO NRs exhibited excitonicrelates ultraviolet (UV) and defect-related green band (GB) emissions. By calculating the UV/GB intensity, the Co 0.08 at.% is the proper atomic percentage to have fewer intrinsic defects. We predict that Co-doped ZnO NRs induce a blueshift of near band edge (NBE) emission due to the Burstein-Moss effect. Meanwhile, the redshift of NBE emission is attributed to the modification of the lattice dimensions and exchange energy.