• Title/Summary/Keyword: band gap

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Effects of the Thickness and the Morphology of a ZnO Buffer Layer in Inverted Organic Solar Cells

  • Lee, Hyeon-U;O, Jin-Yeong;Baek, Hong-Gu
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.151-151
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    • 2013
  • 무기물 기반, Si-based 태양전지에 비해 가볍고 저렴하다는 관점에서 유기태양전지에 대한 연구가 진행되고 있다. 유기태양전지는 Si-based 태양전지에 비해 그 효율이 낮다는 점이 문제로 제기되어 왔지만, 억셉터와 도너의 nanocomposite 구조인 bulk-heterojunction (BHJ) 구조가 개발이 되면서 유기물의 짧은 엑시톤(exciton) 거리를 극복할 수 있게 되어 그 효율이 비약적으로 증가되는 결과를 낳았다. 또한 넓은 범위의 파장을 흡수 할 수 있는 작은 band-gap을 갖는 물질이 개발됨으로써 유기 태양전지의 효율은 점차 증가하고 있다. 최근에는 독일 회사인 Heliatek에서 12%가 넘는 유기태양전지를 발표함으로써 유기태양전지가 Si-based 태양전지를 대체할 수 있는 차세대 에너지 공급원으로의 가능성을 충분히 보였다. 이런 유기 태양전지는 하부 투명전극인 인듐주석산화물(ITO)/정공이동층(PEDOT:PSS)/광흡수층/전자이동층(LiF)/낮은 일함수를 갖는 상부전극인 Al 구조의 일반적인 구조; ITO/전자이동층/광흡수층/정공이동층/높은 일함수를 갖는 상부전극(Ag), 전하의 이동방향이 반대인 역구조 태양전지, 두 가지로 분류할 수 있다. 하지만 소자 안정성의 관점에서 일반적인 구조의 태양전지는 ITO/PEDOT:PSS 계면에서의 화학적 불안정성과, 낮을 일함수를 갖는 상부전극이 쉽게 산화되는 등의 문제가 있어 상부전극으로 높은 일함수를 갖는 전극을 사용하는 역구조 태양전지가 더 유리하다. 이러한 역구조 태양전지에서 효율을 높일 수 있는 요인 중 하나는 전자이동층에 있다. 광흡수층에서 형성되어 분리된 전자가 전극으로 이동하기위해서는 전자이동층을 거쳐야 한다. 하지만 이 전자이동층 내에서의 전자 이동속도가 느리다면, 즉 저항이 크다면 광흡수증과의 계면에서 Back electron trasnfer현상으로 재결합이 일어나게 되어 전극으로 도달하는 전자의 양이 줄어들게 되고, 이는 유기태양전지 효율을 낮추는 요인이 된다. 전자이동층 자체의 저항뿐만 아니라, 전자이동층의 표면 거칠기(morphology) 또한 유기 태양전지의 효율을 좌우하는 요인 중 하나이다. 광흡수층과 전자이동층의 계면에서 전자의 이동이 일어나는데, 전자이동층의 표면 거칠기가 크게되면 그 위에 박막으로 형성되는 광흡수층과의 계면저항이 증가하게 되고, 이는 광흡수층에서 전자이동층으로의 원활한 전자이동을 저해함으로써 소자 효율의 감소를 일으키게 된다. 따라서 우리는 전자이동층인 ZnO 박막의 스퍼터링 조건을 변화시킴으로써 ZnO 층의 두께에 따른 광투과도, 전기전도성 변화 및 유기태양전지의 효율변화와, 표면 거칠기에 따른 광변환 효율 변화를 관찰하고자 한다.

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Cu2ZnSn(S,Se)4 Thin Film Solar Cells Fabricated by Sulfurization of Stacked Precursors Prepared Using Sputtering Process

  • Gang, Myeng Gil;Shin, Seung Wook;Lee, Jeong Yong;Kim, Jin Hyeok
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.97-97
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    • 2013
  • Recently, Cu2ZnSn(S,Se)4 (CZTSS), which is one of the In- and Ga- free absorber materials, has been attracted considerable attention as a new candidate for use as an absorber material in thin film solar cells. The CZTSS-based absorber material has outstanding characteristics such as band gap energy of 1.0 eV to 1.5 eV, high absorption coefficient on the order of 104 cm-1, and high theoretical conversion efficiency of 32.2% in thin film solar cells. Despite these promising characteristics, research into CZTSS based thin film solar cells is still incomprehensive and related reports are quite few compared to those for CIGS thin film solar cells, which show high efficiency of over 20%. I will briefly overview the recent technological development of CZTSS thin film solar cells and then introduce our research results mainly related to sputter based process. CZTSS thin film solar cells are prepared by sulfurization of stacked both metallic and sulfide precursors. Sulfurization process was performed in both furnace annealing system and rapid thermal processing system using S powder as well as 5% diluted H2S gas source at various annealing temperatures ranging from $520^{\circ}C$ to $580^{\circ}C$. Structural, optical, microstructural, and electrical properties of absorber layers were characterized using XRD, SEM, TEM, UV-Vis spectroscopy, Hall-measurement, TRPL, etc. The effects of processing parameters, such as composition ratio, sulfurization pressure, and sulfurization temperature on the properties of CZTSS absorber layers will be discussed in detail. CZTSS thin film solar cell fabricated using metallic precursors shows maximum cell efficiency of 6.9% with Jsc of 25.2 mA/cm2, Voc of 469 mV, and fill factor of 59.1% and CZTS thin film solar cell using sulfide precursors shows that of 4.5% with Jsc of 19.8 mA/cm2, Voc of 492 mV, and fill factor of 46.2%. In addition, other research activities in our lab related to the formation of CZTS absorber layers using solution based processes such as electro-deposition, chemical solution deposition, nano-particle formation will be introduced briefly.

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The investigation of adsorption properties of filter media for removal efficiency of nitrogen, phosphorus using experimental and density functional theory (실험 및 밀도범함수이론을 이용한 질소, 인 저감 효과 분석을 위한 여재의 흡착 특성 연구)

  • Kim, Taeyoon;Kwon, Yongju;Kang, Choonghyun;Kim, Jongyoung;Shin, Hyun Suk;Kwon, Soonchul;Cha, Sung Min
    • Journal of Wetlands Research
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    • v.20 no.3
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    • pp.263-271
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    • 2018
  • In this study, we analyzed the removal efficiency of ammonia nitrogen and phosphate dependant on the column depths using various absorbents such as zeolite silica sand, and activated carbon through the column test. In addition, we analyzed electrochemical adsorption behaviors of ammonia nitrogen and phosphate through the quantum mechanical calculation based on density functional theory calculation. Experimental results represent the removal efficiency of ammonia nitrogen and phosphate are zeolite > activated carbon > silica sand, and activated carbon > zeolite > silica sand, respectively. Zeolite shows high adsorption property for ammonia nitrogen over 90%, regardless of the column depth, while activated carbon exhibits high adsorption property for both ammonia nitrogen and phosphate as the column depth for filter media increases. Theoretical findings using DFT calculation for the adsorption behaviors of adsorbents (activated carbon and silica sand) and nutrients ($PO_4{^{3-}}$, $NH_4{^{+}}$) show that activated carbon represented narrower HOMO-LUMO band gap with high adsorption energy, and even more favorable environment for electron adsorption than silica sand, which leads to the effective removal of nutrients.

Roles of i-SiC Buffer Layer in Amorphous p-SiC/i-SiC/i-Si/n-Si Thin Film Solar Cells (비정질 p-SiC/i-SiC/i-Si/n-Si 박막 태양전지에서 i-SiC 완충층의 역할)

  • Kim, Hyun-Chul;Shin, Hyuck-Jae;Lee, Jae-Shin
    • Korean Journal of Materials Research
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    • v.9 no.12
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    • pp.1155-1159
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    • 1999
  • Thin film solar cells on a glass/$SnO_2$ substrate with p-SiC/i-Si/n-Si heterojunction structures were fabricated using a plasma-enhanced chemical-vapor deposition system. The photovoltaic properties of the solar cells were examined with varying the gas phase composition, x=$CH_4/\;(SiH_4+CH_4)$, during the deposition of the p-SiC layer. In the range of x=0~0.4, the efficiency of solar cell increased because of the increased band gap of the p-SiC window layer. Further increase in the gas phase composition, however, led to a decrease in the cell efficiency probably due to in the increased composition mismatch at the p-SiC/i-Si layers. As a result, the efficiency of a glass/$SnO_2$/p-SiC/i-SiC/i-Si/n-Si/Ag thin film solar cell with $1cm^2$ area was 8.6% ($V_{oc}$=0.85V, $J_{sc}$=16.42mA/$cm^2$, FF=0.615) under 100mW/$cm^2$ light intensity.

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Characteristics of Nickel_Titanium Dual-Metal Schottky Contacts Formed by Over-Etching of Field Oxide on Ni/4H-SiC Field Plate Schottky Diode and Improvement of Process (Ni/4H-SiC Field Plate Schottky 다이오드 제작 시 과도 식각에 의해 형성된 Nickel_Titanium 이중 금속 Schottky 접합 특성과 공정 개선 연구)

  • Oh, Myeong-Sook;Lee, Jong-Ho;Kim, Dae-Hwan;Moon, Jeong-Hyun;Yim, Jeong-Hyuk;Lee, Do-Hyun;Kim, Hyeong-Joon
    • Korean Journal of Materials Research
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    • v.19 no.1
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    • pp.28-32
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    • 2009
  • Silicon carbide (SiC) is a promising material for power device applications due to its wide band gap (3.26 eV for 4H-SiC), high critical electric field and excellent thermal conductivity. The Schottky barrier diode is the representative high-power device that is currently available commercially. A field plate edge-terminated 4H-SiC was fabricated using a lift-off process for opening the Schottky contacts. In this case, Ni/Ti dual-metal contacts were unintentionally formed at the edge of the Schottky contacts and resulted in the degradation of the electrical properties of the diodes. The breakdown voltage and Schottky barrier height (SBH, ${\Phi}_B$) was 107 V and 0.67 eV, respectively. To form homogeneous single-metal Ni/4H-SiC Schottky contacts, a deposition and etching method was employed, and the electrical properties of the diodes were improved. The modified SBDs showed enhanced electrical properties, as witnessed by a breakdown voltage of 635 V, a Schottky barrier height of ${\Phi}_B$=1.48 eV, an ideality factor of n=1.04 (close to one), a forward voltage drop of $V_F$=1.6 V, a specific on resistance of $R_{on}=2.1m{\Omega}-cm^2$ and a power loss of $P_L=79.6Wcm^{-2}$.

A DC-DC Converter Design for OLED Display Module (OLED Display Module용 DC-DC 변환기 설계)

  • Lee, Tae-Yeong;Park, Jeong-Hun;Kim, Jeong-Hoon;Kim, Tae-Hoon;Vu, Cao Tuan;Kim, Jeong-Ho;Ban, Hyeong-Jin;Yang, Gweon;Kim, Hyoung-Gon;Ha, Pan-Bong;Kim, Young-Hee
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.12 no.3
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    • pp.517-526
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    • 2008
  • A one-chip DC-DC converter circuit for OLED(Organic Light-Emitting Diode) display module of automotive clusters is newly proposed. OLED panel driving voltage circuit, which is a charge-pump type, has improved characteristics in miniaturization, low cost and EMI(Electro-Magnetic Interference) compared with DC-DC converter of PWM(Pulse Width Modulator) type. By using bulk-potential biasing circuit, charge loss due to parasitic PNP BJT formed in charge pumping, is prevented. In addition, the current dissipation in start-up circuit of band-gap reference voltage generator is reduced by 42% and the layout area of ring oscillator is reduced by using a logic voltage VLP in ring oscillator circuit using VDD supply voltage. The driving current of VDD, OLED driving voltage, is over 40mA, which is required in OLED panels. The test chip is being manufactured using $0.25{\mu}m$ high-voltage process and the layout area is $477{\mu}m{\times}653{\mu}m$.

Some Conditions of Seeking Happiness: How Can We Feel Happy? (행복의 조건: 우리는 '어떻게' 행복을 느끼는가?)

  • Lee, Eul-sang
    • Journal of Korean Philosophical Society
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    • v.139
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    • pp.133-167
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    • 2016
  • Happiness is no more than a pleasant mental state that we can feel everyday. How to seek happiness is the key subject of positive psychology, for which we also need a clear neural system so that our emotional life can be accomplished. This is an issue in people with neural problems (such as psychopathy or hypochondria) as they can not achieve such emotional clarity. In this sense neuroscience is thought of as a new approach that can replace the traditional rational insight which has been aimed at completing a virtual life. But there is also a limit: we can not reach a virtual life with only a confirmation of our transitive state. A practice of virtue which our moral ethos aims at, has been a problem of rational insight. Here is a gap between our emotional life and our rational insight in which an anguish of psychology results. So a task we should combine organically is band between neuroscientific fact and ethical practice; a new addition to psychology. But unfortunately psychology can not solve this problem by itself, for it is a meta-question arising beyond psychology. Thus an explication of this meta-question is, I believe, a new theory of moral philosophy; one that can only be explored using an interdisciplinary approach.

Microfluidic Assisted Synthesis of Ag-ZnO Nanocomposites for Enhanced Photocatalytic Activity (광촉매 성능 강화를 위한 미세유체공정 기반 Ag-ZnO 나노복합체 합성)

  • Ko, Jae-Rak;Jun, Ho Young;Choi, Chang-Ho
    • Clean Technology
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    • v.27 no.4
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    • pp.291-296
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    • 2021
  • Recently, there has been increasing demand for advancing photocatalytic techniques that are capable of the efficient removal of organic pollutants in water. TiO2, a representative photocatalytic material, has been commonly used as an effective photocatalyst, but it is rather expensive and an alternative is required that will fulfill the requirements of both high performing photocatalytic activities and cost-effectiveness. In this work, ZnO, which is more cost effective than TiO2, was synthesized by using a microreactor-assisted nanomaterials (MAN) process. The process enabled a continuous production of ZnO nanoparticles (NPs) with a flower-like structure with high uniformity. In order to resolve the limited light absorption of ZnO arising from its large band gap, Ag NPs were uniformly decorated on the flower-like ZnO surface by using the MAN process. The plasmonic effect of Ag NPs led to a broadening of the absorption range toward visible wavelengths. Ag NPs also helped inhibit the electron-hole recombination by drawing electrons generated from the light absorption of the flower-like ZnO NPs. As a result, the Ag-ZnO nanocomposites showed improved photocatalytic activities compared with the flower-like ZnO NPs. The photocatalytic activities were evaluated through the degradation of methylene blue (MB) solution. Scanning electron microscopy (SEM), x-ray diffraction (XRD), and energy-dispersive x-ray spectroscopy (EDS) confirmed the successful synthesis of Ag-ZnO nanocomposites with high uniformity. Ag-ZnO nanocomposites synthesized via the MAN process offer the potential for cost-effective and scalable production of next-generation photocatalytic materials.

Synthesis and Photocatalytic Activity of WO3-xFx Photocatalysts Using a Vapor Phase Fluorination (기상 불소화법을 이용한 WO3-xFx 광촉매의 합성 및 광분해 특성)

  • Lee, Hyeryeon;Lim, Chaehun;Lee, Raneun;Lee, Young-Seak
    • Applied Chemistry for Engineering
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    • v.32 no.6
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    • pp.632-639
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    • 2021
  • In this research, fluorine doping was performed to enhance the photocatalytic activities of WO3 which were measured using methylene blue dye. WO3-xFx photocatalyts were prepared by a vaper phase fluorination during a sintering for preparing WO3 photocatalysts from a WCl6 precursor. The bandgap energy of WO3 photocatalysts decreased from 2.95 eV to 2.54 eV, and the oxygen vacancies site increased by about 55% after fluorine doping. In addition, the initial degradation efficiency of methylene blue showed that the fluorine doped sample showed a 6-fold increase in photocatalytic activities from 10% to 60% compared to that of the untreated sample. It is believed that fluorine is doped to reduce the band gap of photocatalysts, enabling the catalytic activity with low energy, and that oxygen vacancies-generated surface defects increase the visible light absorption region of WO3 photocatalysts, thereby increasing photocatalytic activity. In this study, it was confirmed that fluorine-doped WO3-xFx photocatalysts with an excellent photocatalytic activity can be manufactured easily using a one-step vaper phase fluorination that does not require a post-treatment process.

Thermoelectric Properties of the Reaction Sintered n-type β-SiC (반응소결법으로 제조한 n형 β-SiC의 열전특성)

  • Pai, Chul-Hoon
    • Journal of the Korea Academia-Industrial cooperation Society
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    • v.20 no.3
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    • pp.29-34
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    • 2019
  • Silicon carbide is considered to be a potentially useful material for high-temperature electronic devices, as its large energy band gap and the p-type and/or n-type conduction can be controlled by impurity doping. Particularly, electric conductivity of porous n-type SiC semiconductors fabricated from ${\beta}-SiC$ powder at $2000^{\circ}C$ in $N_2$ atmosphere was comparable to or even larger than the reported values of SiC single crystals in the temperature region of $800^{\circ}C$ to $1000^{\circ}C$, while thermal conductivity was kept as low as 1/10 to 1/30 of that for a dense SiC ceramics. In this work, for the purpose of decreasing sintering temperature, it was attempted to fabricate porous reaction-sintered bodies at low temperatures ($1400-1600^{\circ}C$) by thermal decomposition of polycarbosilane (PCS) impregnated in n-type ${\beta}-SiC$ powder. The repetition of the impregnation and sintering process ($N_2$ atmosphere, $1600^{\circ}C$, 3h) resulted in only a slight increase in the relative density but in a great improvement in the Seebeck coefficient and electrical conductivity. However the power factor which reflects the thermoelectric conversion efficiency of the present work is 1 to 2 orders of magnitude lower than that of the porous SiC semiconductors fabricated by conventional sintering at high temperature, it can be stated that thermoelectric properties of SiC semiconductors fabricated by the present reaction-sintering process could be further improved by precise control of microstructure and carrier density.