• 제목/요약/키워드: band gap

검색결과 1,562건 처리시간 0.026초

유 무기 페로브스카이트 태양전지의 열화와 안정성 (Degradation and Stability of Organic-Inorganic Perovskite Solar Cells)

  • 조경진;김성탁;배수현;정태원;이상원;이경동;이승훈;권구한;안세원;이헌민;고민재;강윤묵;이해석;김동환
    • Current Photovoltaic Research
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    • 제4권2호
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    • pp.68-79
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    • 2016
  • The power conversion efficiency of perovskite solar cells has remarkably increased from 3.81% to 22.1% in the past 6 years. Perovskite solar cells, which are based on the perovskite crystal structure, are fabricated using organic-inorganic hybrid materials. The advantages of these solar cells are their low cost and simple fabrication procedure. Also, they have a band gap of about 1.6 eV and effectively absorb light in the visible region. For the commercialization of perovskite solar cells in the field of photovoltaics, the issue of their long term stability cannot be overlooked. Although the development of perovskite solar cells is unprecedented, their main drawback is the degradation of the perovskite structure by moisture. This degradation is accelerated by exposure to UV light, temperature, and external bias. This paper reviews the aforesaid reasons for perovskite solar cell degradation. We also discuss the research directions that can lead to the development of perovskite solar cells with high stability.

TGS법으로 성장한 $In_{l-x}Ga_{x}As$의 특성에 관한 연구 (A study on the Properties of $In_{l-x}Ga_{x}As$ Grown by the TGS Methods)

  • 이원상;문동찬;김선태;서영석
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1988년도 추계학술대회 논문집 학회본부
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    • pp.372-375
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    • 1988
  • The III-V ternary alloy semiconductor $In_{l-x}Ga_{x}As$ were grown by the temperature Gradient of $0.60{\leq}x{\leq}0.98$. The electrical properties were investigated by the Hall effect measurement with the Van der Pauw method in the temperature range of $90{\sim}300K$. $In_{l-x}Ga_{x}As$ were revealed n-type and the carrier concentration at 300K were in the range of $9.69{\times}10^{16}cm^{-3}{\sim}7.49{\times}10^{17}cm^{-3}$. The resistivity was increased and the carrier mobility was decreased with increasing the composition ratio. The optical energy gap determined by optical transmission were $20{\sim}30meV$ lower than theoretical valves on the basis of absorption in the conduction band tail and it was decreased with increasing the temperature by the Varshni rule. In the photoluminescence of undoped $In_{l-x}Ga_{x}As$ at 20K, the main emission was revealed by the radiative recombination of shallow donor(Si) to acceptor(Zn) and the peak energy was increased with increasing the composition, X. The diffusion depth of Zn increases proportionally with the square root of diffusion time, and the activation energy for the Zn diffusion into $In_{0.10}Ga_{0.90}As$ was 2.174eV and temperatures dependence of diffusion coefficient was D = 87.29 exp(-2.174/$K_{B}T$). The Zn diffusion p-n $In_{x}Ga_{x}As$ diode revealed the good rectfying characteristics and the diode factor $\beta{\approx}2$. The electroluminescence spectrum for the Zn-diffusion p-n $In_{0.10}Ga_{0.90}As$ diode was due to radiative recombation between the selectron trap level(${\sim}140meV$) and Zn acceptor level(${\sim}30meV$). The peak energy and FWHM of electroluminescence spectrum at 77K were 1.262eV and 81.0meV, respectively.

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A New Strategy to Fabricate a Colloidal Array Templated $TiO_2$ Photoelectrode for Dye-sensitized Solar Cells

  • 이현정
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2011년도 춘계학술발표대회
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    • pp.8.1-8.1
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    • 2011
  • Nanocrystalline titanium dioxide ($TiO_2$) materials have been widely used as an electron collector in DSSC. This is required to have an extremely high porosity and surface area such that the dye can be sufficiently adsorbed and be electronically interconnected, resulting in the generation of a high photocurrent within cells. In particular, their geometrical structures and crystalline phase have been extensively investigated as important issues in improving its photovoltaic efficiency. In this study, we present a new strategy to fabricate a photoelectrode having a periodic structured $TiO_2$ film templated from 1D or 3D polystyrene (PS) microspheres array. Monodisperse PS spheres of various radiuses were used for colloidal array on FTO glasses and two types of photoelectrode structures with different $TiO_2$ materials were investigated respectively. One is the igloo-shaped electrode prepared by $TiO_2$ deposition by RF-sputtering onto 2D microsphere-templated substrates. At the interface between the film and substrate, there are voids formed by the decomposition of PS microspheres during the calcination step. These holes might be expected to play the predominant roles as scattering spherical voids to promote a light harvesting effect, a spacious structure for electrolytes with higher viscosity and effective paths for electron transfer. Additionally the nanocrystalline $TiO_2$ phase prepared by the RF-sputtering method was previously reported to improve the electron drift mobility within $TiO_2$ electrodes. This yields solar cells with a cell efficiency of 2.45% or more at AM 1.5 illumination, which is a very remarkable result, considering its $TiO_2$ electrode thickness (<2 ${\mu}m$). This study can be expanded to obtain higher cell efficiency by higher dye loading through the increase of surface area or multi-layered stacking. The other is the inverse opal photonic crystal electrode prepared by titania particles infusion within 3D colloidal arrays. To obtain the enlargement of ordered area and high quality of crystallinity, the synthesis of titania particles coated with a organic thin layer were applied instead of sol-gel process using the $TiO_2$ precursors. They were dispersed so well in most solvents without aggregates and infused successfully within colloidal array structures. This ordered mesoporous structure provides the large surface area leading to the enough adsorption of dye molecules and have an light harvesting effect due to the photonic band gap properties (back-and-forth reflection effects within structures). A major advantage of this colloidal array template method is that the pore size and its distribution within $TiO_2$ photoelectrodes are determined by those of latex beads, which can be controlled easily. These materials may have promising potentials for future applications of membrane, sensor and so on as well as solar cells.

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90% $Bi_2Te_3-10% Bi_2Se_3$ 단결정의 밴드갭 에너지와 열전특성 (Band-Gap Energy and Thermoelectric Properties of 90% $Bi_2Te_3-10% Bi_2Se_3$ Single Crystals)

  • 하헌필;현도빈;황종승;오태성
    • 한국재료학회지
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    • 제9권4호
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    • pp.349-354
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    • 1999
  • Dopant를 첨가하지 않은 시료와 donor dopant로 $CdI_2$를 첨가한 $Bi_2Te_3-10%$ 단결정을 Bridgman법으로 성장시키고 Hall 계수, 전하이동도, 전기비저향, Seebeck 계수, 열전도도 빛 성능지수를 77~600K의 온도범위에서 측정하였다. Dopant를 첨가하지 않은 90% $Bi_2Te_3-10% Bi_2Se_3$ 단결정에서 포화정공농도는 $5.85\times10_{18}cm^{-3}$ 이고 degenerate 온도는 127K 이었£며, 전하 이동에 대한 산란인자는 -0.23 이고 전자이동도와 정꽁이동도의 비 ($\mu_e/\mu_h)$는 1.45 이었다. 90% $Bi_2Te_3-10% Bi_2Te_3$ 단결정의 OK 에서의 밴드갭 에너지는 0.200 eV 로서 $Bi_2Te_3-Bi_2Se_3$계 단결정에서눈 $Bi_2Se_3$의 놓도가 증가할수록 밴 드갭 에너지가 증가하였다. Donor dopant로 $CdI_2$를 첨가한 90% $Bi_2Te_3-Bi_2Se_3$ 조성의 n형 단결정에서 성능지수의 최대값은 $CdI_2$를 0.05 wt% 첨가한 경우에 약 230K에서 $3.2\times10^{-3}/K$를 나타내었다.

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전기자동차용 고신뢰성 파워모듈 패키징 기술 (Power Module Packaging Technology with Extended Reliability for Electric Vehicle Applications)

  • 윤정원;방정환;고용호;유세훈;김준기;이창우
    • 마이크로전자및패키징학회지
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    • 제21권4호
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    • pp.1-13
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    • 2014
  • The paper gives an overview of the concepts, basic requirements, and trends regarding packaging technologies of power modules in hybrid (HEV) and electric vehicles (EV). Power electronics is gaining more and more importance in the automotive sector due to the slow but steady progress of introducing partially or even fully electric powered vehicles. The demands for power electronic devices and systems are manifold, and concerns besides aspects such as energy efficiency, cooling and costs especially robustness and lifetime issues. Higher operation temperatures and the current density increase of new IGBT (Insulated Gate Bipolar Transistor) generations make it more and more complicated to meet the quality requirements for power electronic modules. Especially the increasing heat dissipation inside the silicon (Si) leads to maximum operation temperatures of nearly $200^{\circ}C$. As a result new packaging technologies are needed to face the demands of power modules in the future. Wide-band gap (WBG) semiconductors such as silicon carbide (SiC) or gallium nitride (GaN) have the potential to considerably enhance the energy efficiency and to reduce the weight of power electronic systems in EVs due to their improved electrical and thermal properties in comparison to Si based solutions. In this paper, we will introduce various package materials, advanced packaging technologies, heat dissipation and thermal management of advanced power modules with extended reliability for EV applications. In addition, SiC and GaN based WBG power modules will be introduced.

Hot wall epitaxy(HWE)법에 의한 $AgGaSe_2$ 단결정 박막 성장과 열처리 효과 (Growth and effect of thermal annealing for $AgGaSe_2$ single crystal thin film by hot wall epitaxy)

  • 백승남;홍광준;김장복
    • 한국결정성장학회지
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    • 제16권5호
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    • pp.189-197
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    • 2006
  • [$AgGaSe_2$] 단결정 박막을 수평 전기로에서 합성한 $AgGaSe_2$ 다결정을 증발원으로하여, hot wall epitaxy(HWE) 방법으로 증발원과 기판(반절연성-GaAs(100))의 온도를 각각 $630^{\circ}C,\;420^{\circ}C$로 고정하여 성장하였다. 이때 단결정 박막의 결정성은 광발광 스펙트럼과 이중결정 X-선 요동곡선(DCRC)으로 부터 구하였다. $AgGaSe_2$의 광흡수 스펙트럼으로부터 구한 온도에 의존하는 에너지 밴드갭 $E_g(T)$는 Varshni 공식에 fitting한 결과 $E_g(T)=1.9501eV-(8.79x10^{-4}eV/K)T^2(T+250K)$를 잘 만족하였다. 성장된 $AgGaSe_2$ 단결정 박막을 Ag, Ga, Se 분위기에서 각각 열처리하여 10K에서 photoluminescience(PL) spectrum을 측정하여 점 결함의 기원을 알아보았다. PL 측정으로 부터 얻어진 $V_{Ag},\;V_{Se},\;Ag_{int}$, 그리고 $Se_{int}$는 주개와 받개로 분류되어졌다. $AgGaSe_2$ 단결정 박막을 Ag 분위기에서 열처리하면 p형으로 변환됨을 알 수 있었다. 또한, Ga 분위기에서 열처리하면 열처리 이전의 PL 스펙트럼을 보이고 있어서, $AgGaSe_2$ 단결정 박막에서 Ga은 안정된 결합의 형태로 있기 때문에 자연 결함의 형성에는 관련이 없음을 알았다.

Hot Wall Epitaxy(HWE)법에 의한 Cdln2S4 단결정 박막 성장과 열처리 효과 (The Effect of Thermal Annealing and Growth of Cdln2S4 Single Crystal Thin Film by Hot Wall Epitaxy)

  • 홍광준;이관교
    • 한국전기전자재료학회논문지
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    • 제15권11호
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    • pp.923-932
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    • 2002
  • A stoichiometric mixture of evaporating materials for CdIn$\_$2/S$\_$4/ single crystal thin films was prepared from horizontal furnace. To obtain the single crystal thin films, CdIn$\_$2/S$\_$4/ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by hot wall epitaxy(HWE) system. The source and substrate temperatures were 630 $\^{C}$ and 420 $\^{C}$, respectively. The crystalline structure of single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction(DCXD). The carrier density and mobility of CdIn$\_$2/S$\_$4/ single crystal thin films measured from Hall effect by van der Pauw method are 9.01$\times$10$\^$16/ cm$\^$-3/ and 219 ㎠/V$.$s at 293 K, respectively. From the optical absorption measurement, the temperature dependence of energy band gap on CdIn$\_$2/S$\_$4/ single crystal thin films was found to be Eg(T) = 2.7116 eV - (7.74 $\times$ 10$\^$-4/ eV) T$\^$2//(T+434). After the as-grown CdIn$\_$2/S$\_$4/ single crystal thin films was annealed in Cd-, S-, and In-atmospheres, the origin of point defects of CdIn$\_$2/S$\_$4/ single crystal thin films has been investigated by the photoluminescence(PL) at 10 K. The native defects of V$\_$cd/, V$\_$s/, Cd$\_$int/ and S$\_$int/ obtained by PL measurements were classified as donors or accepters type. And we concluded that the heat-treatment in the S-atmosphere converted CdIn$\_$2/S$\_$4/ single crystal thin films to an optical p-type. Also, we confirmed that In in CdIn$\_$2/S$\_$4/GaAs did not from the native defects because In in CdIn$\_$2/S$\_$4/ single crystal thin films existed in the form of stable bonds.

예열 온도 변화에 따른 Sol-Gel 법에 의해 제작된 ZnO 박막의 물리적 특성 연구 (Physical Properties of ZnO Thin Films Grown by Sol-Gel Process with Different Preheating Temperatures)

  • 김익주;한호철;이충선;송용진;태원필;서수정;김용성
    • 한국세라믹학회지
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    • 제41권2호
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    • pp.136-142
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    • 2004
  • 출발물질로 zinc acetate dihydrate(Zn($CH_3$COO)$_2$$.$2$H_2O$)를 사용하였고, 이 물질을 isopropanol(($CH_3$)$_2$CHOH)-monoethanolamine(MEA:H$_2$NCH$_2$C$H_2O$H) 용액에 용해하여 균일하고 안정한 sol을 만들었다. Sol-gel spin-coating 법에 의해 ZnO 박막을 제조시 예열 온도에 따른 박막의 c-축 배향성과 그 물리적 특성을 조사하였다. c-축으로의 성장은 예열 온도의 변화에 따라 차이를 보였으며. 275$^{\circ}C$에서 예열 후 $650^{\circ}C$에서 최종 열처리한 ZnO 박막은 XRD 측정결과 기판에 수직한 (002) 방향으로 강한 배향성을 나타내었다 200∼30$0^{\circ}C$에서 예열 후, $650^{\circ}C$에서 최종 열처리한 ZnO 박막은 UV-vis측정결과 가시광선 영역에서 온도에 따른 투과도의 변화를 보이지만 평균 85% 이상의 높은 투과도를 보였다. 또한 370nm 부근에서 흡수단을 나타내었으며, 광학적 밴드갭은 약 3.22 eV로 나타났다. 발광방출(PL) 측정결과, 황색(620nm, 2.0 eV)발광이 관찰되어, 무기발광 소자로의 응용 가능성을 나타내었다.

Hot Wall Epitaxy(HWE)법에 의한 CdGa2Se4 단결정 박막 성장과 열처리 효과 (The Effect of Thermal Annealing and Growth of CdGa2Se4 Single Crystal Thin Film by Hot Wall Epitaxy)

  • 홍명석;홍광준
    • 한국전기전자재료학회논문지
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    • 제20권10호
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    • pp.829-838
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    • 2007
  • The stochiometric mix of evaporating materials for the $CdGa_2Se_4$ single crystal thin films was prepared from horizontal furnace. To obtain the single crystal thin films, $CdGa_2Se_4$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the Hot Wall Epitaxy (HWE) system. The source and substrate temperature were $630^{\circ}C$ and $420^{\circ}C$, respectively. The crystalline structure of single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD).The carrier density and mobility of $CdGa_2Se_4$ single crystal thin films measured from Hall effect by van der Pauw method are $8.27{\times}10^{17}\;cm^{-3},\;345\;cm^2/V{\cdot}s$ at 293 K. respectively. The temperature dependence of the energy band gap of the $CdGa_2Se_4$ obtained from the absorption spectra was well described by the Varshni's relation, $Eg(T)\;=\;2.6400\;eV\;-\;(7.721{\times}10^{-4}\;eV/K)T^2/(T+399\;K)$. After the as-grown single crystal $CdGa_2Se_4$ thin films were annealed in Cd-, Se-, and Ga -atmospheres, the origin of point defects of single crystal $CdGa_2Se_4$ thin films has been investigated by PL at 10 K. The native defects of $V_{Cd}$, $V_{Se}$, $Cd_{int}$, and $Se_{int}$ obtained by PL measurements were classified as donors or accepters. We concluded that the heat-treatment in the Cd-atmosphere converted single crystal $CdGa_2Se_4$ thin films to an optical p-type. Also, we confirmed that Ga in $CdGa_2Se_4/GaAs$ did not form the native defects because Ga in single crystal $CdGa_2Se_4$ thin films existed in the form of stable bonds.

n-ZnO/i-ZnO/p-GaN:Mg 이종접합을 이용한 UV 발광 다이오드 (Ultraviolet LEDs using n-ZnO:Ga/i-ZnO/p-GaN:Mg heterojunction)

  • 한원석;김영이;공보현;조형균;이종훈;김홍승
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2008년도 추계학술대회 논문집 Vol.21
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    • pp.50-50
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    • 2008
  • ZnO has been extensively studied for optoelectronic applications such as blue and ultraviolet (UV) light emitters and detectors, because it has a wide band gap (3.37 eV) anda large exciton binding energy of ~60 meV over GaN (~26 meV). However, the fabrication of the light emitting devices using ZnO homojunctions is suffered from the lack of reproducibility of the p-type ZnO with high hall concentration and mobility. Thus, the ZnO-based p-n heterojunction light emitting diode (LED) using p-Si and p-GaN would be expected to exhibit stable device performance compared to the homojunction LED. The n-ZnO/p-GaN heterostructure is a good candidate for ZnO-based heterojunction LEDs because of their similar physical properties and the reproducibleavailability of p-type GaN. Especially, the reduced lattice mismatch (~1.8 %) and similar crystal structure result in the advantage of acquiring high performance LED devices with low defect density. However, the electroluminescence (EL) of the device using n-ZnO/p-GaN heterojunctions shows the blue and greenish emissions, which are attributed to the emission from the p-GaN and deep-level defects. In this work, the n-ZnO:Ga/p-GaN:Mg heterojunction light emitting diodes (LEDs) were fabricated at different growth temperatures and carrier concentrations in the n-type region. The effects of the growth temperature and carrier concentration on the electrical and emission properties were investigated. The I-V and the EL results showed that the device performance of the heterostructure LEDs, such as turn-on voltage and true ultraviolet emission, developed through the insertion of a thin intrinsic layer between n-ZnO:Ga and p-GaN:Mg. This observation was attributed to a lowering of the energy barriers for the supply of electrons and holes into intrinsic ZnO, and recombination in the intrinsic ZnO with the absence of deep level emission.

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