• Title/Summary/Keyword: Ga)Se_2$

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Growth and Optical Conductivity Properties for BaAl2Se4 Single Crystal Thin Film by Hot Wall Epitaxy (Hot Wall Epitaxy(HWE)법에 의한 BaAl2Se4 단결정 박막 성장과 광전도 특성)

  • Jeong, Junwoo;Lee, Kijung;Hong, Kwangjoon
    • Journal of Sensor Science and Technology
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    • v.24 no.6
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    • pp.404-411
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    • 2015
  • A stoichiometric mixture of evaporating materials for $BaAl_2Se_4$ single crystal thin films was prepared from horizontal electric furnace. To obtain the single crystal thin films, $BaAl_2Se_4$ 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 $610^{\circ}C$ 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 $BaAl_2Se_4$ single crystal thin films measured from Hall effect by van der Pauw method are $8.29{\times}10^{-16}cm^{-3}$ and $278cm^2/vs$ at 293 K, respectively. The temperature dependence of the energy band gap of the $BaAl_2Se_4$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)=3.4205eV-(4.3112{\times}10^{-4}eV/K)T^2/(T+232 K)$. The crystal field and the spin-orbit splitting energies for the valence band of the $BaAl_2Se_4$ have been estimated to be 249.4 meV and 263.4 meV, 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 $BaAl_2Se_4/GaAs$ epilayer. The three photocurrent peaks observed at 10 K are ascribed to the $A_1$-, $B_1$-exciton for n =1 and $C_{31}$-exciton peaks for n=31.

Growth and temperature dependence of energy band gap for $CuAISe_2$ Single Crystal Thin Film by Hot Wall Epitaxy (Hot Wall Epitaxy(HWE)법에 의한 $CuAlSe_2$ 단결정 박막의 성장과 에너지 밴드갭의 온도 의존성)

  • Yun, Seok-Jin;Hong, Kwang-Joon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.06a
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    • pp.121-122
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    • 2007
  • Single crystal $CuAlSe_2$ layers were grown on thoroughly etched sem-insulating GaAs(l00) substrate at $410^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating $CuAlSe_2$ source at $680^{\circ}C$. 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 single crystal $CuAlSe_2$ thin films measured with Hall effect by van der Pauw method are $9.24{\times}l0^{16}\;cm^{-3}$ and $295\;cm^2/V{\cdot}s$ at 293K, 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, $E_g(T)\;=\;2.8382\;eV\;-\;(8.68\;{\times}\;10^{-4}\;eV/K)T^2/(T\;+\;155\;K)$.

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Effect of the Concentration of Citrate on the Growth of Aqueous Chemical Bath Deposited ZnO and Application of the Film to Cu(In,Ga)Se2 Solar Cells (Citrate 농도에 따른 수용액 화학조 증착 ZnO 성장 및 ZnO 박막의 Cu(In,Ga)Se2 태양전지 응용)

  • Cho, Kyung Soo;Jang, Hyunjun;Oh, Jae-Young;Kim, Jae Woo;Lee, Jun Su;Choi, Yesol;Hong, Ki-Ha;Chung, Choong-Heui
    • Korean Journal of Materials Research
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    • v.30 no.4
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    • pp.204-210
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    • 2020
  • ZnO thin films are of considerable interest because they can be customized by various coating technologies to have high electrical conductivity and high visible light transmittance. Therefore, ZnO thin films can be applied to various optoelectronic device applications such as transparent conducting thin films, solar cells and displays. In this study, ZnO rod and thin films are fabricated using aqueous chemical bath deposition (CBD), which is a low-cost method at low temperatures, and environmentally friendly. To investigate the structural, electrical and optical properties of ZnO for the presence of citrate ion, which can significantly affect crystal form of ZnO, various amounts of the citrate ion are added to the aqueous CBD ZnO reaction bath. As a result, ZnO crystals show a nanorod form without citrate, but a continuous thin film when citrate is above a certain concentration. In addition, as the citrate concentration increases, the electrical conductivity of the ZnO thin films increases, and is almost unchanged above a certain citrate concentration. Cu(In,Ga)Se2 (CIGS) solar cell substrates are used to evaluate whether aqueous CBD ZnO thin films can be applicable to real devices. The performance of aqueous CBD ZnO thin films shows performance similar to that of a sputter-deposited ZnO:Al thin film as top transparent electrodes of CIGS solar cells.

Molybdenum Oxides as Diffusion Barrier Layers against MoSe2 Formation in A Nonvacuum Process for CuInSe2 Solar Cells (비진공법 CuInSe2 태양전지에서 MoSe2의 생성을 억제하기 위한 산화 몰리브데늄 확산장벽 층)

  • Lee, Byung-Seok;Lee, Doh-Kwon
    • Current Photovoltaic Research
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    • v.3 no.3
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    • pp.85-90
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    • 2015
  • Two-step processes for preparing $Cu(In,Ga)Se_2$ absorber layers consist of precursor layer formation and subsequent annealing in a Se-containing atmosphere. Among the various deposition methods for precursor layer, the nonvacuum (wet) processes have been spotlighted as alternatives to vacuum-based methods due to their potential to realize low-cost, scalable PV devices. However, due to its porous nature, the precursor layer deposited on Mo substrate by nonvacuum methods often suffers from thick $MoSe_2$ formation during selenization under a high Se vapor pressure. On the contrary, selenization under a low Se pressure to avoid $MoSe_2$ formation typically leads to low crystal quality of absorber films. Although TiN has been reported as a diffusion barrier against Se, the additional sputtering to deposit TiN layer may induce the complexity of fabrication process and nullify the advantages of nonvacuum deposition of absorber film. In this work, Mo oxide layers via thermal oxidation of Mo substrate have been explored as an alternative diffusion barrier. The morphology and phase evolution was examined as a function of oxidation temperature. The resulting Mo/Mo oxides double layers were employed as a back contact electrode for $CuInSe_2$ solar cells and were found to effectively suppress the formation of $MoSe_2$ layer.

Study on Electrical Properties and Temperature Dependence of Energy Band Gap for $ZnIn_2Se_4$ Single Crystal Thin Film Grown by Hot Wall Epitaxy (뜨겨운 곁쌓기법에 의해 성장된 $ZnIn_2Se_4$ 단결정 박막의 전기적 특성과 에너지 갭의 온도 의존성)

  • Park, Hyang-Sook
    • Journal of Integrative Natural Science
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    • v.3 no.1
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    • pp.54-59
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    • 2010
  • A stoichiometric mixture of evaporating materials for $ZnIn_2Se_4$ single crystal thin films was prepared from horizontal electric furnace. To obtain the single crystal thin films, $ZnIn_2Se_4$ 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 $630^{\circ}C$ and $400^{\circ}C$, 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 $ZnIn_2Se_4$ single crystal thin films measured from Hall effect by van der Pauw method are $9.41{\times}10^{16}cm^{-3}$ and $292cm^2/v{\cdot}s$ at 293 K, respectively. The temperature dependence of the energy band gap of the $ZnIn_2Se_4$ obtained from the absorption spectra was well described by the Varshni's relation, $Eg(T)=1.8622eV-(5.23{\times}10^{-4}eV/K)T^2/(T+775.5K)$.

Preparation of CIGSe thin film solar cells by solution process and selenization

  • Park, Mi-Seon;Jo, Hyo-Jeong;Seong, Si-Jun;Hwang, Dae-Gyu;Kim, Dae-Hwan;Gang, Jin-Gyu
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.410-410
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    • 2011
  • Chalcopyrite계 화합물 $CuInGaSe_2$($CIGSe_2$)는 높은 광흡수율과 전기적 특성 및 안정성, 그리고 1.02~1.67 eV 범위의 최적의 에너지 밴드갭을 가져 박막태양전지용 광흡수층 재료로 많은 관심을 받고 있다. 일반적으로 $CIGSe_2$ 박막태양전지의 광흡수층을 형성하는 공정은 고효율 태양전지 제작이 가능한 진공공정을 이용한다. $CIGSe_2$ 광흡수층을 형성하는데 있어 진공 공정을 용액기반 공정으로 대처한다면 저비용으로 보다 간단하면서 효율적인 태양전지의 제조가 가능 할 것으로 기대된다. 본 연구에서는 $CIGSe_2$ 광흡수층을 2 단계에 걸쳐 제작하였다. 먼저 Cu, In, Ga 성분을 포함하는 용액을 이용하여 CIG 전구체막을 형성한 후, 다음 단계로 selenization 공정을 진행함으로써 $CIGSe_2$ 박막을 제작하였다. $CIGSe_2$의 결정 성장을 위하여 selenization 공정의 열처리 온도와 시간을 조절하여 CIG 전구체막과 Se 원소의 결합반응을 최적화할 수 있는 공정 조건을 확보하였으며 이를 통해 우수한 결정 및 전기적 특성을 갖는 $CIGSe_2$박막을 제조하였다. 제작된 $CIGSe_2$ 박막의 광전변환 효율을 측정하여 단위셀로서의 구현이 가능함을 확인하였으며 XRD, SEM, EDS, UV-visible을 통하여 $CIGSe_2$박막의 특성을 분석하였다.

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Thermal diffusion properties of Zn, Cd, S, and B at the interface of CuInGaSe2 solar cells

  • Yoon, Young-Gui;Choi, In-Hwan
    • Current Photovoltaic Research
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    • v.1 no.1
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    • pp.52-58
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    • 2013
  • Two different window-structured $CuInGaSe_2$(CIGS) solar cells, i.e., CIGS/thin-CdS/ZnO:B(sample A) and CIGS/very thin-CdS/Zn(S/O)/ZnO:B(sample B), were prepared, and the diffusivity of Zn, Cd, S, and B atoms, respectively, in the CIGS, ZnO or Zn(S/O) layer was estimated by a theoretical fit to experimental secondary ion mass spectrometer data. Diffusivities of Zn, Cd, S, and B atoms in CIGS were $2.0{\times}10^{-13}(1.5{\times}10^{-13})$, $4.6{\times}10^{-13}(4.4{\times}10^{-13})$, $1.6{\times}10^{-13}(1.8{\times}10^{-13})$, and $1.2{\times}10^{-12}cm^2/s$ at 423K, respectively, where the values in parentheses were obtained from sample B and the others from sample A. The diffusivity of the B atom in a Zn(S/O) of sample B was $2.1{\times}10^{-14}cm^2/sec$. Moreover, the diffusivities of Cd and S atoms diffusing back into ZnO(sample A) or Zn(S/O)(sample A) layers were extremely low at 423K, and the estimated diffusion coefficients were $2.2{\times}10^{-15}cm^2/s$ for Cd and $3.0{\times}10^{-15}cm^2/s$ for S.

The Operating Temperature Effects on GaAs Solar Cells (CaAs 해양전지의 온도특성)

  • Lee, Seung-Ki;Han, Min-Koo;Chung, Gi-Oong;Kwon, Young-Se
    • Proceedings of the KIEE Conference
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    • 1987.11a
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    • pp.203-206
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    • 1987
  • $Ga_{1-x}Al_xAs$ solar cells have been fabricated by LPE and characterized as a function of operating temperature from $25^{\circ}C$ to $l30^{\circ}C$. Open circuit voltage decreases linearly with increasing temperature by $1.4mv/^{\circ}C$, while degradation of silicon solar cells is about $2.2-2.5\;mv/^{\circ}C$. Experimental results regarding to GaAS solar cells, such as saturation current, ideality factors and fill factors are characterized as a function of operating temperature.

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GaAs-Carbon Nanotubes Nanocomposite: Synthesis and Field-Emission Property (갈륨비소-탄소나노튜브 복합체 제작과 전계방출특성)

  • Lim, Hyun-Chul;Chandrasekar, P.V.;Chang, Dong-Mi;Ahn, Se-Yong;Jung, Hyuk;Kim, Do-Jin
    • Korean Journal of Materials Research
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    • v.20 no.4
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    • pp.199-203
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    • 2010
  • Hybridization of semiconductor materials with carbon nanotubes (CNTs) is a recent field of interest in which new nanodevice fabrication and applications are expected. In this work, nanowire type GaAs structures are synthesized on porous single-wall carbon nanotubes (SWCNTs) as templates using the molecular beam epitaxy (MBE) technique. The field emission properties of the as-synthesized products were investigated to suggest their potential applications as cold electron sources, as well. The SWCNT template was synthesized by the arc-discharge method. SWCNT samples were heat-treated at $400^{\circ}C$ under an $N_2/O_2$ atmosphere to remove amorphous carbon. After heat treatment, GaAs was grown on the SWCNT template. The growth conditions of the GaAs in the MBE system were set by changing the growth temperatures from $400^{\circ}C$ to $600^{\circ}C$. The morphology of the GaAs synthesized on the SWCNTs strongly depends on the substrate temperature. Namely, nano-crystalline beads of GaAs are formed on the CNTs under $500^{\circ}C$, while nanowire structures begin to form on the beads above $600^{\circ}C$. The crystal qualities of GaAs and SWCNT were examined by X-ray diffraction and Raman spectra. The field emission properties of the synthesized GaAs nanowires were also investigated and a low turn-on field of $2.0\;V/{\mu}m$ was achieved. But, the turn-on field was increased in the second and third measurements. It is thought that arsenic atoms were evaporated during the measurement of the field emission.